Optical filter and imaging apparatus

ABSTRACT

An optical ( 1   a ) includes a light-absorbing layer ( 10 ). The light-absorbing layer absorbs light in at least a portion of the near-infrared region. When light with a wavelength of 300 to 1200 nm is incident on the optical filter ( 1   a ) at an incident angle of 0°, the optical filter ( 1   a ) satisfies given spectral transmittance requirements. When an average of absolute values of differences each between a value of a normalized spectral transmittance for an incident angle x° and a value of a normalized spectral transmittance for an incident angle y° in the wavelength range of W nm to V nm (W&lt;V) is expressed as ΔT S   x/y   W-V , the optical filter ( 1   a ) satisfies requirements ΔT S   0/40   380-530 ≤3%, ΔT S   0/40   450-650 ≤3%, and ΔT S   0/40   530-750 ≤3%.

TECHNICAL FIELD

The present invention relates to an optical filter and an imaging apparatus.

BACKGROUND ART

Imaging apparatuses including an optical filter such as a near-infrared cut filter are conventionally known. For example, Patent Literature 1 describes a near-infrared cut filter including a laminated sheet having a near-infrared-absorber-including resin layer provided on at least one side of a glass sheet substrate. For example, this near-infrared cut filter has a dielectric multilayer film provided on at least one side of the laminated sheet. For this near-infrared cut filter, the absolute value |Ya−Yb| of the difference between a wavelength value (Ya) and a wavelength value (Yb) is less than 15 nm. The wavelength value (Ya) is a value of a wavelength which lies in the wavelength range of 560 to 800 nm and at which the transmittance measured in the direction perpendicular to the near-infrared cut filter is 50%. The wavelength value (Yb) is a value of a wavelength which lies in the wavelength range of 560 to 800 nm and at which the transmittance measured at an incident angle of 30° to the near-infrared cut filter is 50%. As just described, the dependence of the transmission characteristics of the near-infrared cut filter according to Patent Literature 1 on the incident angle of light is adjusted to be small.

Patent Literature 2 describes a near-infrared cut filter including a near-infrared-absorbing glass substrate, near-infrared-absorbing layer, and dielectric multilayer film. The near-infrared-absorbing layer includes a near-infrared-absorbing dye and transparent resin. Patent Literature 2 describes a solid-state imaging apparatus including this near-infrared cut filter and a solid-state imaging device. According to Patent Literature 2, the influence of the incident angle dependence which dielectric multilayer films inherently have and which is dependence of a shift of a blocking wavelength on the incident angle of light can be almost completely eliminated by laminating the near-infrared-absorbing glass substrate and near-infrared-absorbing layer. For example, in Patent Literature 2, a transmittance (T₀) at an incident angle of 0° and a transmittance (T₃₀) at an incident angle of 30° are measured for the near-infrared cut filter.

Patent Literatures 3 and 4 each describe an infrared cut filter including a transparent dielectric substrate, an infrared-reflecting layer, and an infrared-absorbing layer. The infrared-reflecting layer is formed of a dielectric multilayer film. The infrared-absorbing layer includes an infrared-absorbing dye. Patent Literatures 3 and 4 each describe an imaging apparatus including this infrared cut filter. Patent Literatures 3 and 4 each describe transmittance spectra shown by the infrared cut filter for light incident at incident angles of 0°, 25°, and 35°.

CITATION LIST

Patent Literature

Patent Literature 1: JP 2012-103340 A

Patent Literature 2: WO 2014/030628 A1

Patent Literature 3: JP 2014-52482 A

Patent Literature 4: JP 2014-203044 A

SUMMARY OF INVENTION Technical Problem

The above patent literatures fail to specifically discuss the characteristics which would be exhibited by the optical filters when light is incident on the optical filters at an incident angle larger than 35° (e.g., 40° or larger). Therefore, the present invention provides an optical filter that can block unnecessary light and that exhibits advantageous characteristics for preventing uneven coloring of an image generated by an imaging apparatus even when the incident angle of light is larger. The present invention also provides an imaging apparatus including this optical filter.

Solution to Problem

The present invention provides an optical filter, including

a light-absorbing layer that includes a light absorber for absorbing light in at least a portion of the near-infrared region, wherein

when light with a wavelength of 300 to 1200 nm is incident on the optical filter at an incident angle of 0°, the optical filter satisfies the following requirements (1) to (9):

(1) a spectral transmittance at a wavelength of 380 nm is 20% or less;

(2) the spectral transmittance at a wavelength of 450 nm is 75% or more;

(3) an average of the spectral transmittance in the wavelength range of 500 to 600 nm is 80% or more;

(4) the spectral transmittance at a wavelength of 700 nm is 5% or less;

(5) the spectral transmittance at a wavelength of 715 nm is 3% or less;

(6) an average of the spectral transmittance in the wavelength range of 700 to 800 nm is 1% or less;

(7) the maximum of the spectral transmittance in the wavelength range of 750 to 1080 nm is 1% or less;

(8) the maximum of the spectral transmittance in the wavelength range of 1000 to 1100 nm is 2% or less; and

(9) a wavelength bandwidth of a wavelength band in which the spectral transmittance in the wavelength range of 400 to 700 nm is 75% or more is 170 nm or more, and

when light with a wavelength of 300 to 1200 nm is incident on the optical filter at incident angles of x° and y° (0≤x≤30, 30≤y≤65, and x<y) and an average of absolute values of differences each between a value of a normalized spectral transmittance for the incident angle x° and a value of a normalized spectral transmittance for the incident angle y° at the same wavelength in the wavelength range of W nm to V nm (W<V) is expressed as ΔT_(S) ^(x/y) _(W-V),

the optical filter satisfies requirements ΔT_(S) ^(0/40) ₃₈₀₋₅₃₀≤3%, ΔT_(S) ^(0/40) ₄₅₀₋₆₅₀≤3%, and ΔT_(S) ^(0/40) ₅₃₀₋₇₅₀≤3%,

the normalized spectral transmittance being determined by normalization of a spectral transmittance for each of the incident angles so that the maximum of the spectral transmittance for each of the incident angles in the wavelength range of 400 to 650 nm is 100%.

The present invention also provides an imaging apparatus including:

a lens system;

an imaging device that receives light having been transmitted through the lens system; and

the above optical filter that is disposed ahead of the imaging device.

Advantageous Effects of Invention

The above optical filter can block unnecessary light and exhibits advantageous characteristics for preventing uneven coloring of an image generated by an imaging apparatus even when the incident angle of light is larger. Moreover, an image generated by the above imaging apparatus of the present invention is unlikely to be colored unevenly.

BRIEF DESCRIPTION OF DRAWINGS

FIG. 1A is a cross-sectional view of an example of an optical filter of the present invention.

FIG. 1B is a cross-sectional view of another example of the optical filter of the present invention.

FIG. 1C is a cross-sectional view of yet another example of the optical filter of the present invention.

FIG. 1D is a cross-sectional view of yet another example of the optical filter of the present invention.

FIG. 1E is a cross-sectional view of yet another example of the optical filter of the present invention.

FIG. 2 is a cross-sectional view showing an example of an imaging apparatus according to the present invention.

FIG. 3A shows transmittance spectra shown by an optical filter according to Example 1 for light incident at incident angles of 0°, 3°, 35°, and 40°.

FIG. 3B shows transmittance spectra shown by the optical filter according to Example 1 for light incident at incident angles of 45°, 50°, 55°, 60°, and 65°.

FIG. 4A shows normalized transmittance spectra shown by the optical filter according to Example 1 for light incident at incident angles of 0°, 30°, 35°, and 40°.

FIG. 4B shows normalized transmittance spectra shown by the optical filter according to Example 1 for light incident at incident angles of 45°, 50°, 55°, 60°, and 65°.

FIG. 5A shows transmittance spectra shown by an optical filter according to Example 2 for light incident at incident angles of 0°, 30°, 35°, and 40°.

FIG. 5B shows transmittance spectra shown by the optical filter according to Example 2 for light incident at incident angles of 45°, 50°, 55°, 60°, and 65°.

FIG. 6A shows normalized transmittance spectra shown by the optical filter according to Example 2 for light incident at incident angles of 0°, 30°, 35°, and 40°.

FIG. 6B shows normalized transmittance spectra shown by the optical filter according to Example 2 for light incident at incident angles of 45°, 50°, 55°, 60°, and 65°.

FIG. 7A shows transmittance spectra shown by an optical filter according to Example 3 for light incident at incident angles of 0°, 30°, 35°, and 40°.

FIG. 7B shows transmittance spectra shown by the optical filter according to Example 3 for light incident at incident angles of 45°, 50°, 55°, 60°, and 65°.

FIG. 8A shows normalized transmittance spectra shown by the optical filter according to Example 3 for light incident at incident angles of 0°, 30°, 35°, and 40°.

FIG. 8B shows normalized transmittance spectra shown by the optical filter according to Example 3 for light incident at incident angles of 45°, 50°, 55°, 60°, and 65°.

FIG. 9A shows a transmittance spectrum shown by an intermediate product of an optical filter according to Example 4 for light incident at an incident angle of 0°.

FIG. 9B shows a transmittance spectrum shown by another intermediate product of the optical filter according to Example 4 for light incident at an incident angle of 0°.

FIG. 9C shows a transmittance spectrum shown by a laminate according to

Reference Example 1 for light incident at an incident angle of 0°.

FIG. 9D shows transmittance spectra shown by a laminate according to Reference Example 2 for light incident at incident angles of 0°, 30°, 50°, and 65°.

FIG. 10A shows transmittance spectra shown by the optical filter according to Example 4 for light incident at incident angles of 0°, 3°, 35°, and 40°.

FIG. 10B shows transmittance spectra shown by the optical filter according to Example 4 for light incident at incident angles of 45°, 50°, 5°, 60°, and 65°.

FIG. 11A shows normalized transmittance spectra shown by the optical filter according to Example 4 for light incident at incident angles of 0°, 30°, 35°, and 40°.

FIG. 11B shows normalized transmittance spectra shown by the optical filter according to Example 4 for light incident at incident angles of 45°, 50°, 55°, 60°, and 65°.

FIG. 12A shows transmittance spectra shown by an intermediate product of an optical filter according to Comparative Example 1 for light incident at incident angles of 0°, 30°, and 50°.

FIG. 12B shows a transmittance spectrum shown by a laminate according to Reference Example 3 for light incident at an incident angle of 0°.

FIG. 13A shows transmittance spectra shown by the optical filter according to Comparative Example 1 for light incident at incident angles of 0°, 30°, 35°, and 40°.

FIG. 13B shows transmittance spectra shown by the optical filter according to Comparative Example 1 for light incident at incident angles of 45°, 50°, 55°, 60°, and 65°.

FIG. 14A shows normalized transmittance spectra shown by the optical filter according to Comparative Example 1 for light incident at incident angles of 0°, 30°, 35°, and 40°.

FIG. 14B shows normalized transmittance spectra shown by the optical filter according to Comparative Example 1 for light incident at incident angles of 45°, 50°, 55°, 60°, and 65°.

FIG. 15A shows a transmittance spectrum shown by a light-absorbing transparent substrate used for fabrication of an optical filter according to Comparative Example 2 for light incident at an incident angle of 0°.

FIG. 15B shows transmittance spectra shown by a laminate according to Reference Example 4 for light incident at incident angles of 0°, 30°, and 50°.

FIG. 15C shows a transmittance spectrum shown by a laminate according to Reference Example 5 for light incident at an incident angle of 0°.

FIG. 16A shows transmittance spectra shown by the optical filter according to Comparative Example 2 for light incident at incident angles of 0°, 30°, 35°, and 40°.

FIG. 16B shows transmittance spectra shown by the optical filter according to Comparative Example 2 for light incident at incident angles of 45°, 50°, 55°, 60°, and 65°.

FIG. 17A shows normalized transmittance spectra shown by the optical filter according to Comparative Example 2 for light incident at incident angles of 0°, 30°, 35°, and 40°.

FIG. 17B shows normalized transmittance spectra shown by the optical filter according to Comparative Example 2 for light incident at incident angles of 45°, 50°, 55°, 60°, and 65°.

DESCRIPTION OF EMBODIMENTS

Hereinafter, embodiments of the present invention will be described with reference to the drawings. The following description is directed to some examples of the present invention, and the present invention is not limited by these examples.

The present inventors have invented the optical filter according to the present invention based on new findings obtained from the following studies of optical filters.

An optical filter blocking against unnecessary light other than visible light is disposed in a camera module or imaging apparatus mounted in a personal digital assistant such as a smartphone. The use of an optical filter including a light-absorbing layer has been discussed to block unnecessary light. Like the optical filters described in Patent Literatures 1 to 4, many optical filters including a light-absorbing layer further include a light-reflecting layer composed of a dielectric multilayer film.

Interference of light reflecting on the front and back surfaces of each layer of a light-reflecting layer composed of a dielectric multilayer film determines a wavelength band of transmitted light and a wavelength band of reflected light. Light can be incident on the optical filter at various incident angles. As the incident angle of light gets larger, the optical path length in each layer of the light-reflecting layer changes. As a result, a phenomenon is observed in which the wavelength band of transmitted light and the wavelength band of reflected light shift to the short wavelength side. Therefore, it is conceivable that when light in a given wavelength band is reflected by the light-reflecting layer that is a dielectric multilayer film, a boundary between a wavelength band of light to be blocked and a wavelength band of light to be transmitted is determined by a wavelength band of light absorption so that the transmittance characteristics of the optical filter do not greatly vary depending on the incident angle of light.

In Patent Literatures 1 and 2, the light transmission characteristics of the near-infrared cut filters for light incident at incident angles of 0° and 30° are evaluated. In Patent Literatures 3 and 4, transmittance spectra shown by the infrared cut filters for light incident at incident angles of 0°, 25°, and 35° are evaluated. In recent years, camera modules and imaging apparatuses mounted in personal digital assistants such as smartphones have been expected to achieve a wider angle of view and a much lower profile. Therefore, it is desirable that light transmission characteristics of optical filters be unlikely to vary even when the incident angle of light is larger (e.g., 40° or larger).

In these points of view, for example, it is conceivable that an optical filter is designed so that a dielectric multilayer film will have a boundary between a wavelength band of transmitted light and a wavelength band of reflected light at a wavelength sufficiently longer than a wavelength at which a light-absorbing layer has a boundary between a wavelength band of transmitted light and a wavelength band of absorbed light. In this case, the boundary between the wavelength band of light to be transmitted through the optical filter and a wavelength band of light to be blocked by the optical filter is prevented from shifting to the short wavelength side even when the incident angle of light is larger. However, when the incident angle of light is much larger, the amount of change in optical path length in each layer of the light-reflecting layer increases and, depending on the incident angle of light, a defect called a ripple, which is a local increase in light reflectance and a local decrease in transmittance, can happen in a wavelength band of light to be transmitted. In particular, even an optical filter designed to be free of ripples at incident angles of 0° to 35° may suffer a ripple at an incident angle of 40° or larger. Occurrence of a ripple greatly decreases the sensitivity of an imaging apparatus to light with a certain wavelength to lower than the sensitivity thereof to light with other wavelengths and may cause uneven coloring of an image obtained therewith.

Under these circumstances, the present inventors went through much trial and error to develop an optical filter that can block unnecessary light and that is advantageous for preventing uneven coloring of an image generated by an imaging apparatus even when the incident angle of light is larger. As a result, the present inventors have found that desirable characteristics can be imparted to an optical filter by a given light absorbing layer without combined use of a light-reflecting layer composed of a dielectric multilayer, and thus invented the optical filter according to the present invention.

Herein, the term “spectral transmittance” refers to a transmittance obtained when light with a given wavelength is incident on an object such as a specimen and the term “average transmittance” refers to an average of the spectral transmittance in a given wavelength range. Additionally, the term “transmittance spectrum” herein refers to one in which spectral transmittance values at wavelengths in a given wavelength range are arranged in the wavelength order.

As shown in FIG. 1A, the optical filter 1 a includes a light-absorbing layer 10. The light-absorbing layer 10 includes a light absorber. The light absorber absorbs light in at least a portion of the near-infrared region. When light with a wavelength of 300 to 1200 nm is incident on the optical filter 1 a at an incident angle of 0°, the optical filter 1 a satisfies the following requirements (1) to (9):

(1) a spectral transmittance at a wavelength of 380 nm is 20% or less;

(2) the spectral transmittance at a wavelength of 450 nm is 75% or more;

(3) an average of the spectral transmittance in the wavelength range of 500 to 600 nm is 80% or more;

(4) the spectral transmittance at a wavelength of 700 nm is 5% or less;

(5) the spectral transmittance at a wavelength of 715 nm is 3% or less;

(6) an average of the spectral transmittance in the wavelength range of 700 to 800 nm is 1% or less;

(7) the maximum of the spectral transmittance in the wavelength range of 750 to 1080 nm is 1% or less;

(8) the maximum of the spectral transmittance in the wavelength range of 1000 to 1100 nm is 2% or less; and

(9) a wavelength bandwidth of a wavelength band in which the spectral transmittance in the wavelength range of 400 to 700 nm is 75% or more is 170 nm or more.

As to the above requirement (9), when a plurality of discrete wavelength bands in which the spectral transmittance is 75% or more exists in the wavelength range of 400 to 700 nm, the sum of the wavelength bandwidths of the plurality of wavelength bands is defined as “wavelength bandwidth”.

When light with a wavelength of 300 to 1200 nm is incident on the optical filter 1 a at incident angles of x° and y° (0≤x≤30, 30≤y≤65, and x<y), an average of absolute values of differences each between a value of a normalized spectral transmittance for the incident angle x° and a value of a normalized spectral transmittance for the incident angle y° at the same wavelength in the wavelength range of W nm to V nm (W<V) is expressed as ΔT_(S) ^(x/y) _(W-V). In this case, the optical filter 1 a satisfies requirements ΔT_(S) ^(0/40) ₃₈₀₋₅₃₀≤3%, ΔT_(S) ^(0/40) ₄₅₀₋₆₅₀≤3%, and ΔT_(S) ^(0/40) ₅₃₀₋₇₅₀≤3%.

The normalized spectral transmittance mentioned above is determined by normalization of a spectral transmittance for each of the incident angles so that the maximum of the spectral transmittance for each of the incident angles in the wavelength range of 400 to 650 nm will be 100%. Typically, light with a wavelength of 300 to 1200 nm is allowed to be incident on the optical filter 1 a at incident angles of 0°, 30°, 35°, 40°, 45°, 50°, 55°, 60°, and 65°, and the spectral transmittance is measured at every 1 nm in the wavelength range of 300 to 1200 nm. For the spectral transmittance thus measured at each incident angle, the spectral transmittance value at each wavelength is divided by the maximum of the spectral transmittance in the wavelength range of 400 to 650 nm, and the resultant value is expressed in percentage. A normalized spectral transmittance is thus determined.

Since the optical filter 1 a has the above characteristics, the optical filter 1 a can appropriately block unnecessary light such as light in the near-infrared region without a light-reflecting layer composed of a dielectric multilayer film. The optical filter 1 a may appropriately block light in the ultraviolet region as well. Because of the absence of a light-reflecting layer composed of a dielectric multilayer film from the optical filter 1 a, no ripple occurs in a wavelength band of light to be transmitted even when the incident angle of light is large, and an image generated by an imaging apparatus including the optical filter 1 a is unlikely to be colored unevenly. Additionally, for the optical filter 1 a, the boundary between a wavelength band of transmitted light and a wavelength band of blocked light is prevented from shifting to the short wavelength side with increase in incident angle of light. Since the optical filter 1 a satisfies the requirements ΔT_(S) ^(0/40) ₃₈₀₋₅₃₀≤3%, ΔT_(S) ^(0/40) ₄₅₀₋₆₅₀≤3%, and ΔT_(S) ^(0/40) ₅₃₀₋₇₅₀≤3%, a gap between the shape of a normalized spectral transmittance curve for an incident angle of 0° and the shape of a normalized spectral transmittance curve for an incident angle of 40° is small in the wavelength ranges of 380 to 530 nm, 450 to 650 nm, and 530 to 750 nm.

It is conceivable that the optical filter 1 a is used, for example, when a color filter (hereinafter referred to as “RGB color filter”) consisting of R (red), G (green), and B (blue) segments is disposed at each pixel of an imaging device such as a charge-coupled device (CCD) or complementary metal oxide semiconductor (CMOS). In this case, output from each pixel of the imaging device is appropriately adjusted by the optical filter 1 a, and spectral sensitivity characteristics corresponding to the output from each pixel of the imaging device are likely to well conform to the visual sensitivity.

An optical filter that blocks unnecessary light is commonly disposed with its principal surface parallel to a light receiving surface of an imaging device near the optical filter. In this case, light incident on the optical filter and then on the imaging device is incident on the optical filter and the imaging device at a substantially equal incident angle. A chief ray is incident near the center of an imaging device at an incident angle of nearly 0° while a chief ray incident on the peripheral portion of the imaging device at a large incident angle. Therefore, in the case where the shape of a spectral sensitivity curve changes depending on the incident angle of light incident on an imaging apparatus, the central portion and the peripheral portion of an image taken with the imaging apparatus differ in color when the image is displayed or printed. Therefore, an object expected to be colored with one color in the image is likely to gradually discolor from the central portion toward the peripheral portion, and the discoloration is likely to be recognized as color unevenness. Additionally, in the case where the shape of the spectral sensitivity curve changes in a narrow incident angle range, e.g., 5° to 10°, discoloration is likely to occur in a narrow area on the resultant image and is particularly likely to be recognized as color unevenness. If an incident angle-dependent change in the shape of a normalized spectral transmittance curve can be reduced by means of the optical filter, the incident angle-dependent change in the shape of the spectral sensitivity curve can be reduced and uneven coloring of an image generated by the imaging apparatus can be prevented.

The optical filter 1 a desirably further satisfies a requirement ΔT_(S) ^(0/40) ₆₅₀₋₁₂₀₀≤1%. In this case, the gap between the shape of the normalized spectral transmittance curve for an incident angle of 0° and the shape of a normalized spectral transmittance curve for an incident angle of 40° is small also in the wavelength range of 650 to 1200 nm.

The optical filter 1 a desirably further satisfies a requirement ΔT_(S) ^(0/40) ₃₈₀₋₁₂₀₀≤1.5%. In this case, the gap between the shape of the normalized spectral transmittance curve for an incident angle of 0° and the shape of a normalized spectral transmittance curve for an incident angle of 40° is small over the wavelength range of 380 to 1200 nm.

The wavelength range of 380 to 530 nm corresponds to the wavelength range referred to to determine sensitivity characteristics of a sub-pixel corresponding to a B (blue) filter segment of an RGB color filter incorporated in or disposed near an imaging device. The wavelength range of 450 to 650 nm corresponds to the wavelength range referred to to determine sensitivity characteristics of a sub-pixel corresponding to a G (green) filter segment of an RGB color filter incorporated in or disposed near an imaging device. The wavelength range of 530 to 750 nm corresponds to the wavelength range referred to to determine sensitivity characteristics of a sub-pixel corresponding to an R (red) filter segment of an RGB color filter incorporated in or disposed near an imaging device. The wavelength range of 650 to 1200 nm corresponds to the wavelength range of near-infrared light to be blocked. The wavelength range of 380 to 1200 nm includes the above wavelength ranges and corresponds to the wavelength range referred to to determine the brightness of light that a camera module or an imaging apparatus takes in through the optical filter.

The optical filter 1 a desirably further satisfies requirements ΔT_(S) ^(0/50) ₃₈₀₋₅₃₀≤4%, ΔT_(S) ^(0/50) ₄₅₀₋₆₅₀≤4%, ΔT_(S) ^(0/50) ₅₃₀₋₇₅₀≤4%, ΔT_(S) ^(0/50) ₆₅₀₋₁₂₀₀≤1.5%, and ΔT_(S) ^(0/50) ₃₈₀₋₁₂₀₀≤2%. In this case, a gap between the shape of the normalized spectral transmittance curve for an incident angle of 0° and the shape of a normalized spectral transmittance curve for an incident angle of 50° is small. This makes it easy to prevent uneven coloring of an image generated by an imaging apparatus even when light is incident on the optical filter 1 a included in the imaging apparatus at an incident angle of 50°.

The optical filter 1 a desirably further satisfies requirements ΔT_(S) ^(0/60) ₃₈₀₋₅₃₀≤4.5%, ΔT_(S) ^(0/60) ₄₅₀₋₆₅₀≤4.5%, ΔT_(S) ^(0/60) ₅₃₀₋₇₅₀≤4.5%, ΔT_(S) ^(0/60) ₆₅₀₋₁₂₀₀≤1.5%, and ΔT_(S) ^(0/60) ₃₈₀₋₁₂₀₀≤2.5%. In this case, a gap between the shape of the normalized spectral transmittance curve for an incident angle of 0° and the shape of a normalized spectral transmittance curve for an incident angle of 60° is small. This makes it easy to prevent uneven coloring of an image generated by an imaging apparatus even when light is incident on the optical filter 1 a included in the imaging apparatus at an incident angle of 60°.

The optical filter 1 a desirably further satisfies requirements ΔT_(S) ^(0/65) ₃₈₀₋₅₃₀≤5%, ΔT_(S) ^(0/65) ₄₅₀₋₆₅₀≤5%, ΔT_(S) ^(0/65) ₅₃₀₋₇₅₀≤5%, ΔT_(S) ^(0/65) ₆₅₀₋₁₂₀₀≤1.5%, and ΔT_(S) ^(0/65) ₃₈₀₋₁₂₀₀≤3%. In this case, a gap between the shape of the normalized spectral transmittance curve for an incident angle of 0° and the shape of a normalized spectral transmittance curve for an incident angle of 65° is small. This makes it easy to prevent uneven coloring of an image generated by an imaging apparatus even when light is incident on the optical filter 1 a included in the imaging apparatus at an incident angle of 65°. For example, when an imaging apparatus capable of taking images using a wide-angle lens having a wide angle of view includes the optical filter 1 a, it is easy to prevent uneven coloring of an image taken using the wide-angle lens.

In the case where a wide-angle lens is used in an imaging apparatus, the incident angle of light incident on a light receiving surface of an imaging device can be reduced by certain design of the lens. It is inevitable, however, that light incident on a cover glass located ahead of the lens of the imaging apparatus includes light incident at a large incident angle. When the optical filter 1 a satisfies the above requirements, an image generated by an imaging apparatus including the optical filter 1 a as a cover glass is unlikely to be colored unevenly. Additionally, the optical filter 1 a functioning also as a cover glass can reduce the number of components of the imaging apparatus and makes it easy to achieve a lower-profile imaging apparatus. Besides, in that case, the freedom of lens design is expanded. Moreover, flare and ghost caused by reflection on a principal surface of a conventional optical filter disposed independently of a cover glass can be prevented.

The optical filter 1 a desirably further satisfies requirements ΔT_(S) ^(30/40) ₃₈₀₋₅₃₀≤3%, ΔT_(S) ^(30/40) ₄₅₀₋₆₅₀≤3%, ΔT_(S) ^(30/40) ₅₃₀₋₇₅₀≤3%, ΔT_(S) ^(30/40) ₆₅₀₋₁₂₀₀≤1%, and ΔT_(S) ^(30/40) ₃₈₀₋₁₂₀₀≤1.5%. In this case, a gap between the shape of the normalized spectral transmittance curve for an incident angle of 30° and the shape of the normalized spectral transmittance curve for an incident angle of 40° is small.

The optical filter 1 a desirably further satisfies requirements ΔT_(S) ^(30/50) ₃₈₀₋₅₃₀≤3%, ΔT_(S) ^(30/50) ₄₅₀₋₆₅₀≤3%, ΔT_(S) ^(30/50) ₅₃₀₋₇₅₀≤3%, ΔT_(S) ^(30/50) ₆₅₀₋₁₂₀₀≤1%, and ΔT_(S) ^(30/50) ₃₈₀₋₁₂₀₀≤1.5%. In this case, a gap between the shape of the normalized spectral transmittance curve for an incident angle of 30° and the shape of the normalized spectral transmittance curve for an incident angle of 50° is small.

The optical filter 1 a desirably further satisfies requirements ΔT_(S) ^(30/60) ₃₈₀₋₅₃₀≤4%, ΔT_(S) ^(30/60) ₄₅₀₋₆₅₀≤4%, ΔT_(S) ^(30/60) ₅₃₀₋₇₅₀≤4%, ΔT_(S) ^(30/60) ₆₅₀₋₁₂₀₀≤1.5%, and ΔT_(S) ^(30/60) ₃₈₀₋₁₂₀₀≤2%. In this case, a gap between the shape of the normalized spectral transmittance curve for an incident angle of 30° and the shape of the normalized spectral transmittance curve for an incident angle of 60° is small.

The optical filter 1 a desirably further satisfies requirements ΔT_(S) ^(30/65) ₃₈₀₋₅₃₀≤4.5%, ΔT_(S) ^(30/65) ₄₅₀₋₆₅₀≤4.5%, ΔT_(S) ^(30/65) ₅₃₀₋₇₅₀≤4.5%, ΔT_(S) ^(30/65) ₆₅₀₋₁₂₀₀≤1.5%, and ΔT_(S) ^(30/65) ₃₈₀₋₁₂₀₀≤2.5%. In this case, a gap between the shape of the normalized spectral transmittance curve for an incident angle of 30° and the shape of the normalized spectral transmittance curve for an incident angle of 65° is small.

When the incident angle x° of light is 0°, values of ΔT_(S) ^(0/y) _(W-V) v of the optical filter 1 a desirably satisfy the requirements shown in Table 1.

TABLE 1 ΔTs^(0/y)W-V y = 30° y = 35° y = 40° y = 45° y = 50° y = 55° y = 60° y = 65° W = 380 nm; V = 530 nm   ≤3%   ≤3%   ≤3% ≤4%   ≤4% ≤4.5% ≤4.5%   ≤5% W = 450 nm; V = 650 nm   ≤3%   ≤3%   ≤3% ≤4%   ≤4% ≤4.5% ≤4.5%   ≤5% W = 530 nm; V = 750 nm   ≤3%   ≤3%   ≤3% ≤4%   ≤4% ≤4.5% ≤4.5%   ≤5% W = 650 nm; V = 1200 nm   ≤1%   ≤1%   ≤1% ≤1% ≤1.5% ≤1.5% ≤1.5% ≤1.5% W = 380 nm; V = 1200 nm ≤1.5% ≤1.5% ≤1.5% ≤2%   ≤2% ≤2.5% ≤2.5%   ≤3%

When the incident angle x° of light is 30°, values of ΔT_(S) ³⁰/y_(W-V) of the optical filter 1 a desirably satisfy the requirements shown in Table 2.

TABLE 2 ΔTs^(30/y)W-V y = 35° y = 40° y = 45° y = 50° y = 55° y = 60° y = 65° W = 380 nm; V = 530 nm   ≤3%   ≤3%   ≤3%   ≤3% ≤4%   ≤4% ≤4.5% W = 450 nm; V = 650 nm   ≤3%   ≤3%   ≤3%   ≤3% ≤4%   ≤4% ≤4.5% W = 530 nm; V = 750 nm   <3%   ≤3%   ≤3%   ≤3% ≤4%   ≤4% ≤4.5% W = 650 nm; V = 1200 nm   ≤1%   ≤1%   ≤1%   ≤1% ≤1% ≤1.5% ≤1.5% W = 380 nm; V = 1200 nm ≤1.5% ≤1.5% ≤1.5% ≤1.5% ≤2%   ≤2% ≤2.5%

The light absorber included in the light-absorbing layer 10 is not particularly limited as long as the light absorber absorbs light in at least a portion of the near-infrared region and the optical filter 1 a satisfies the above requirements (1) to (9) and the requirements ΔT_(S) ^(0/40) ₃₈₀₋₅₃₀≤3%, ΔT_(S) ^(0/40) ₄₅₀₋₆₅₀≤3%, and ΔT_(S) ^(0/40) ₅₃₀₋₇₅₀≤3%. The light absorber is, for example, formed by a phosphonic acid and copper ion. In this case, light in a wide wavelength band covering the near-infrared region and a portion of the visible region adjacent to the near-infrared region can be absorbed by the light-absorbing layer 10. Therefore, the desired characteristics can be exhibited even when the optical filter 1 a does not include a light-reflecting layer.

When the light-absorbing layer 10 includes the light absorber formed by a phosphonic acid and copper ion, the phosphonic acid includes, for example, a first phosphonic acid having an aryl group. In the first phosphonic acid, the aryl group is bonded to a phosphorus atom. Thus, the above requirements are easily satisfied by the optical filter 1 a.

The aryl group of the first phosphonic acid is, for example, a phenyl group, benzyl group, toluyl group, nitrophenyl group, hydroxyphenyl group, halogenated phenyl group in which at least one hydrogen atom of a phenyl group is substituted by a halogen atom, or halogenated benzyl group in which at least one hydrogen atom of a benzene ring of a benzyl group is substituted by a halogen atom.

When the light-absorbing layer 10 includes the light absorber formed by the phosphonic acid and copper ion, the phosphonic acid desirably further includes a second phosphonic acid having an alkyl group. In the second phosphonic acid, the alkyl group is bonded to a phosphorus atom.

The alkyl group of the second phosphonic acid is, for example, an alkyl group having 6 or less carbon atoms. This alkyl group may be linear or branched.

When the light-absorbing layer 10 includes the light absorber formed by the phosphonic acid and copper ion, the light-absorbing layer 10 further includes, for example, a phosphoric acid ester allowing the light absorber to be dispersed and matrix resin. The light-absorbing layer 10 further includes, if necessary, a hydrolytic polycondensation product of an alkoxysilane monomer.

The phosphoric acid ester included in the light-absorbing layer 10 is not limited to any particular one, as long as the phosphoric acid ester allows good dispersion of the light absorber. For example, the phosphoric acid ester includes at least one of a phosphoric acid diester represented by the following formula (c1) and a phosphoric acid monoester represented by the following formula (c2). In the formulae (c1) and (c2), R₂₁, R₂₂, and R₃ are each a monovalent functional group represented by —(CH₂CH₂O)_(n)R₄, wherein n is an integer of 1 to 25 and R₄ is an alkyl group having 6 to 25 carbon atoms. R₂₁, R₂₂, and R₃ may be the same or different functional groups.

The phosphoric acid ester is not particularly limited. The phosphoric acid ester can be, for example, PLYSURF A208N (polyoxyethylene alkyl (C12, C13) ether phosphoric acid ester), PLYSURF A208F (polyoxyethylene alkyl (C8) ether phosphoric acid ester), PLYSURF A208B (polyoxyethylene lauryl ether phosphoric acid ester), PLYSURF A219B (polyoxyethylene lauryl ether phosphoric acid ester), PLYSURF AL (polyoxyethylene styrenated phenylether phosphoric acid ester), PLYSURF A212C (polyoxyethylene tridecyl ether phosphoric acid ester), or PLYSURF A215C (polyoxyethylene tridecyl ether phosphoric acid ester). All of these are products manufactured by DKS Co., Ltd. The phosphoric acid ester can be NIKKOL DDP-2 (polyoxyethylene alkyl ether phosphoric acid ester), NIKKOL DDP-4 (polyoxyethylene alkyl ether phosphoric acid ester), or NIKKOL DDP-6 (polyoxyethylene alkyl ether phosphoric acid ester). All of these are products manufactured by Nikko Chemicals Co., Ltd.

The matrix resin included in the light-absorbing layer 10 is, for example, a heat-curable or ultraviolet-curable resin in which the light absorber is dispersible. Additionally, as the matrix resin can be used a resin that has a transmittance of, for example, 80% or more, preferably 85% or more, and more preferably 90% or more for light with a wavelength of 350 nm to 900 nm in the form of a 0.1-mm-thick resin layer. The matrix resin is not limited to a particular resin as long as the optical filter 1 a satisfies the above requirements (1) to (9) and the requirements ΔT_(S) ^(0/40) ₃₈₀₋₅₃₀≤3%, ΔT_(S) ^(0/40) ₄₅₀₋₆₅₀≤3%, and ΔT_(S) ^(0/40) ₅₃₀₋₇₅₀≤3%. The content of the phosphonic acid in the light-absorbing layer 10 is, for example, 3 to 180 parts by mass with respect to 100 parts by mass of the matrix resin.

The matrix resin included in the light-absorbing layer 10 is, for example, a (poly)olefin resin, polyimide resin, polyvinyl butyral resin, polycarbonate resin, polyamide resin, polysulfone resin, polyethersulfone resin, polyamideimide resin, (modified) acrylic resin, epoxy resin, or silicone resin. The matrix resin may contain an aryl group such as a phenyl group and is desirably a silicone resin containing an aryl group such as a phenyl group. If the light-absorbing layer 10 is excessively hard, the likelihood of cure shrinkage-induced cracking during the production process of the optical filter 1 a increases with increasing thickness of the light-absorbing layer 10. When the matrix resin is a silicone resin containing an aryl group, the light-absorbing layer 10 is likely to have high crack resistance. Moreover, with the use of a silicone resin containing an aryl group, the light absorber formed by the above phosphonic acid and copper ion is less likely to be aggregated when included. Further, when the matrix resin of the light-absorbing layer 10 is a silicone resin containing an aryl group, it is desirable for the phosphoric acid ester included in the light-absorbing layer 10 to have a flexible, linear organic functional group, such as an oxyalkyl group, just as does the phosphoric acid ester represented by the formula (c1) or formula (c2). This is because interaction derived from the combination of the above phosphonic acid, a silicone resin containing an aryl group, and phosphoric acid ester having a linear organic functional group such as an oxyalkyl group makes aggregation of the light absorber less likely and can impart good rigidity and good flexibility to the light-absorbing layer. Specific examples of the silicone resin available as the matrix resin include KR-255, KR-300, KR-2621-1, KR-211, KR-311, KR-216, KR-212, KR-251, and KR-5230. All of these are silicone resins manufactured by Shin-Etsu Chemical Co., Ltd.

Examples of the hydrolytic polycondensation product of an alkoxysilane monomer, the hydrolytic polycondensation product possibly being included in the optical filter 1 a, include hydrolytic polycondensation products of the following alkoxysilane monomers. The alkoxysilane monomers are tetramethoxysilane, tetraethoxysilane, methyltrimethoxysilane, methyltriethoxysilane, dimethyldiethoxysilane, dimethyldimethoxysilane, phenyltrimethoxysilane, phenyltriethoxysilane, 3-glycidoxypropyltrimethoxysilane, 3-glycidoxypropyltriethoxysilane, and 3-glycidoxypropylmethyldiethoxysilane.

As shown in FIG. 1A, the optical filter 1 a further includes, for example, a transparent dielectric substrate 20. One principal surface of the transparent dielectric substrate 20 is covered with the light-absorbing layer 10. The characteristics of the transparent dielectric substrate 20 are not particularly limited as long as the optical filter 1 a satisfies the above requirements (1) to (9) and the requirements ΔT_(S) ^(0/40) ₃₈₀₋₅₃₀≤3%, ΔT_(S) ^(0/40) ₄₅₀₋₆₅₀≤3%, and ΔT_(S) ^(30/40) ₅₃₀₋₇₅₀≤3%. The transparent dielectric substrate 20 is, for example, a dielectric substrate having a high average transmittance (for example, 80% or more, preferably 85% or more, and more preferably 90% or more) in the wavelength range of 450 nm to 600 nm.

The transparent dielectric substrate 20 is, for example, made of glass or resin. When the transparent dielectric substrate 20 is made of glass, the glass is, for example, borosilicate glass such as D 263 T eco, soda-lime glass (blue plate glass), white sheet glass such as B 270, alkali-free glass, or infrared-absorbing glass such as copper-containing phosphate glass or copper-containing fluorophosphate glass. When the transparent dielectric substrate 20 is made of infrared-absorbing glass such as copper-containing phosphate glass or copper-containing fluorophosphate glass, the desired infrared absorption performance can be imparted to the optical filter 1 a by a combination of the infrared absorption performance of the transparent dielectric substrate 20 and the infrared absorption performance of the light-absorbing layer 10. Examples of such an infrared-absorbing glass include BG-60, BG-61, BG-62, BG-63, and BG-67 manufactured by SCHOTT AG, 500EXL manufactured by Nippon Electric Glass Co., Ltd., and CM5000, CM500, C5000, and C500S manufactured by HOYA CORPORATION. Moreover, the transparent dielectric substrate 20 may have ultraviolet absorption characteristics.

The transparent dielectric substrate 20 may be a transparent crystalline substrate, such as magnesium oxide, sapphire, or quartz. For example, sapphire is very hard and is thus scratch resistant. Therefore, as a scratch-resistant protective material such as a protective filter or cover glass in an imaging apparatus, a sheet-shaped sapphire is sometimes disposed ahead of a camera module or lens included in mobile devices such as smartphones and mobile phones. Formation of the light-absorbing layer 10 on such a sheet-shaped sapphire makes it possible to protect camera modules and lenses and cut off unnecessary light such as near infrared light.

When the transparent dielectric substrate 20 is made of resin, the resin is, for example, a (poly)olefin resin, polyimide resin, polyvinyl butyral resin, polycarbonate resin, polyamide resin, polysulfone resin, polyethersulfone resin, polyamideimide resin, (modified) acrylic resin, epoxy resin, or silicone resin.

The optical filter 1 a can be produced, for example, by applying a coating liquid for forming the light-absorbing layer 10 to one principal surface of the transparent dielectric substrate 20 to form a film and drying the film. The method for preparing the coating liquid and the method for producing the optical filter 1 a will be described with an example in which the light-absorbing layer 10 includes the light absorber formed by the phosphonic acid and copper ion.

First, an exemplary method for preparing the coating liquid will be described. A copper salt such as copper acetate monohydrate is added to a given solvent such as tetrahydrofuran (THF), followed by stirring to obtain a copper salt solution. To this copper salt solution is then added a phosphoric acid ester compound such as a phosphoric acid diester represented by the formula (c1) or a phosphoric acid monoester represented by the formula (c2), followed by stirring to prepare a solution A. The first phosphonic acid is added to a given solvent such as THF, followed by stirring to prepare a solution B. When the solution B includes a plurality of first phosphonic acids, the solution B may be prepared by adding each of the phosphonic acids to a given solvent such as THF, stirring each of the resultant mixtures, and mixing the plurality of liquids thus prepared. When the optical filter 1 a includes the hydrolytic polycondensation product of the alkoxysilane monomer, for example, the alkoxysilane monomer is further added to prepare the solution B.

Next, the solution B is added to the solution A while the solution A is stirred, and the mixture is further stirred for a given period of time. To the resultant solution is then added a given solvent such as toluene, followed by stirring to obtain a solution C. Subsequently, the solution C is subjected to solvent removal under heating for a given period of time to obtain a solution D. This process removes the solvent such as THF and the component such as acetic acid (boiling point: about 118° C.) generated by disassociation of the copper salt and yields a light absorber formed by the first phosphonic acid and copper ion. The temperature at which the solution C is heated is chosen based on the boiling point of the to-be-removed component disassociated from the copper salt. During the solvent removal, the solvent such as toluene (boiling point: about 110° C.) used to obtain the solution C is also evaporated. A certain amount of this solvent desirably remains in the coating liquid. This is preferably taken into account in determining the amount of the solvent to be added and the time period of the solvent removal. To obtain the solution C, o-xylene (boiling point: about 144° C.) may be used instead of toluene. In this case, the amount of o-xylene to be added can be reduced to about one-fourth of the amount of toluene to be added, because the boiling point of o-xylene is higher than the boiling point of toluene. A matrix resin such as a silicone resin is added to the solution D, followed by stirring. The coating liquid can thus be prepared.

The coating liquid is applied to one principal surface of the transparent dielectric substrate 20 to form a film. For example, the coating liquid is applied to one principal surface of the transparent dielectric substrate 20 by die coating or spin coating or with a dispenser to form a film. Next, this film is cured by a given heat treatment. For example, the film is exposed to an environment at a temperature of 50° C. to 200° C. for a given period of time.

The coating liquid may further contain the second phosphonic acid. In this case, the coating liquid is prepared, for example, by mixing and stirring the solution D, a solution H containing the second phosphonic acid, and a matrix resin. The solution H can be prepared, for example, in the following manner.

A copper salt such as copper acetate monohydrate is added to a given solvent such as tetrahydrofuran (THF), followed by stirring to obtain a copper salt solution. To this copper salt solution is then added a phosphoric acid ester compound such as a phosphoric acid diester represented by the formula (c1) or a phosphoric acid monoester represented by the formula (c2), followed by stirring to prepare a solution E. The second phosphonic acid is added to a given solvent such as THF, followed by stirring to prepare a solution F. Next, the solution F is added to the solution E while the solution E is stirred, and the mixture is further stirred for a given period of time. To the resultant solution is then added a given solvent such as toluene, followed by stirring to obtain a solution G. Subsequently, the solution G is subjected to solvent removal under heating for a given period of time to obtain a solution H.

The light-absorbing layer 10 of the optical filter 1 a may be formed as a single layer or may be formed as a plurality of layers. When the light-absorbing layer 10 is formed as a plurality of layers, the light-absorbing layer 10 includes, for example, a first layer including the light absorber formed by the first phosphonic acid and copper ion and a second layer including the light absorber formed by the second phosphonic acid and copper ion. In this case, a coating liquid for forming the first layer can be obtained by adding a matrix resin such as a silicone resin to the solution D and stirring the mixture. The second layer is formed using a coating liquid prepared separately from the coating liquid for forming the first layer. The coating liquid for forming the second layer can be obtained, for example, by adding a matrix resin such as a silicone resin to the solution H and stirring the mixture.

The first and second layers can be formed by applying the coating liquid for forming the first layer and that for forming the second layer to form films, which are cured by a given heat treatment. For example, the films are exposed to an environment at a temperature of 50° C. to 200° C. for a given period of time. The order of forming the first and second layers is not particularly limited. The first and second layers may be formed in different time periods, or may be formed in the same time period. A protective layer may be formed between the first and second layers. The protective layer is formed of, for example, a SiO₂-deposited film.

Modifications

The optical filter 1 a can be modified in various respects. For example, the optical filter 1 a may be modified to optical filters 1 b to 1 e shown in FIG. 1B to FIG. 1E. The optical filters 1 b to 1 e are configured in the same manner as the optical filter 1 a, unless otherwise described. The components of the optical filters 1 b to 1 e that are the same as or correspond to those of the optical filter 1 a are denoted by the same reference characters, and detailed descriptions of such components are omitted. The description given for the optical filter 1 a can apply to the optical filters 1 b to 1 e, unless there is technical inconsistency.

As shown in FIG. 1B, the optical filter 1 b has the light-absorbing layers 10 formed on both principal surfaces of the transparent dielectric substrate 20. Therefore, the above requirements (1) to (9) and the requirements ΔT_(S) ^(0/40) ₃₈₀₋₅₃₀≤3%, ΔT_(S) ^(0/40) ₄₅₀₋₆₅₀≤3%, and ΔT_(S) ^(0/40) ₅₃₀₋₇₅₀≤3% are satisfied not by one light-absorbing layer 10 but by the two light-absorbing layers 10 separated by the transparent dielectric substrate 20. The light-absorbing layers 10 on both principal surfaces of the transparent dielectric substrate 20 may have the same or different thicknesses. That is, the formation of the light-absorbing layers 10 on both principal surfaces of the transparent dielectric substrate 20 is done so that the two light-absorbing layers 10 account for equal or unequal proportions of the light-absorbing layer thickness required for the optical filter 1 b to have desired optical characteristics. Thus, each of the light-absorbing layers 10 formed on both principal surfaces of the transparent dielectric substrate 20 of the optical filter 1 b has a smaller thickness than the thickness of the light-absorbing layer 10 of the optical filter 1 a. The formation of the light-absorbing layers 10 on both principal surfaces of the transparent dielectric substrate 20 can reduce warping of the optical filter 1 b even when the transparent dielectric substrate 20 is thin. Each of the two light-absorbing layers 10 may be formed as a plurality of layers.

As shown in FIG. 1C, the optical filter 1 c has the light-absorbing layers 10 formed on both principal surfaces of the transparent dielectric substrate 20. The optical filter 1 c additionally includes an anti-reflection film 30. The anti-reflection film 30 is a film formed as an interface between the optical filter 1 c and air and reducing reflection of visible light. The anti-reflection film 30 is, for example, a film formed of a dielectric made of, for example, a resin, an oxide, or a fluoride. The anti-reflection film 30 may be a multilayer film formed by laminating two or more types of dielectrics having different refractive indices. The anti-reflection film 30 may be, particularly, a dielectric multilayer film made of a low-refractive-index material such as SiO₂ and a high-refractive-index material such as TiO₂ or Ta₂O₅. In this case, Fresnel reflection at the interface between the optical filter 1 c and air is reduced and the amount of visible light transmitted through the optical filter 1 c can be increased. The anti-reflection film 30 may be formed on both sides of the optical filter 1 c, or may be formed on one side thereof.

As shown in FIG. 1D, the optical filter 1 d consists only of the light-absorbing layer 10. The optical filter 1 d can be produced, for example, by applying the coating liquid onto a given substrate such as a glass substrate, resin substrate, or metal substrate (such as a steel substrate or stainless steel substrate) to form a film, curing the film, and then separating the film from the substrate. The optical filter 1 d may be produced by casting. Not including the transparent dielectric substrate 20, the optical filter 1 d is thin. The optical filter 1 d can thus contribute more to achievement of lower-profile imaging apparatuses.

As shown in FIG. 1E, the optical filter 1 e includes the light-absorbing layer 10 and a pair of the anti-reflection films 30 disposed on both sides of the light-absorbing layer 10. In this case, the optical filter 1 e can contribute to achievement of lower-profile imaging apparatuses and can increase the amount of visible light transmitted therethrough more than the optical filter 1 d can.

The optical filters 1 a to 1 e may be modified to include an infrared-absorbing layer (not shown) in addition to the light-absorbing layer 10, if necessary. The infrared-absorbing layer includes, for example, an organic infrared absorber, such as a cyanine-based, phthalocyanine-based, squarylium-based, diimmonium-based, or azo-based infrared absorber or an infrared absorber composed of a metal complex. The infrared-absorbing layer includes, for example, one infrared absorber or two or more infrared absorbers selected from these infrared absorbers. The organic infrared absorber can absorb light in a relatively narrow wavelength range (absorption band) and is suitable for absorbing light with a given wavelength range.

The optical filters 1 a to 1 e may be modified to include an ultraviolet-absorbing layer (not shown) in addition to the light-absorbing layer 10, if necessary. The ultraviolet-absorbing layer includes, for example, an ultraviolet absorber, such as a benzophenone-based, triazine-based, indole-based, merocyanine-based, or oxazole-based ultraviolet absorber. The ultraviolet-absorbing layer, for example, includes one ultraviolet absorber or two or more ultraviolet absorbers selected from these ultraviolet absorbers. The ultraviolet absorber can include ultraviolet absorbers that absorbs ultraviolet light with a wavelength around, for example, 300 nm to 340 nm, emits light (fluorescence) with a wavelength longer than the absorbed wavelength, and functions as a fluorescent agent or fluorescent brightener. The ultraviolet-absorbing layer can reduce incidence of ultraviolet light which deteriorates the materials, such as resin, used in the optical filter.

The above infrared absorber and/or ultraviolet absorber may be contained beforehand in the transparent dielectric substrate 20 made of resin to form a substrate having characteristics of absorbing infrared light and/or ultraviolet light. In this case, it is necessary for the resin to allow the infrared absorber and/or ultraviolet absorber to be appropriately dissolved or dispersed therein and be transparent. Examples of such a resin include a (poly)olefin resin, polyimide resin, polyvinyl butyral resin, polycarbonate resin, polyamide resin, polysulfone resin, polyethersulfone resin, polyamideimide resin, (modified) acrylic resin, epoxy resin, and silicone resin.

As shown in FIG. 2 , the optical filter 1 a is used to produce, for example, an imaging apparatus 100 (camera module). The imaging apparatus 100 includes a lens system 2, an imaging device 4, and the optical filter 1 a. Since the optical filter 1 a satisfies the above requirements (1) to (9) and the requirements ΔT_(S) ^(0/40) ₃₈₀₋₅₃₀≤3%, ΔT_(S) ^(0/40) ₄₅₀₋₆₅₀≤3%, and ΔT_(S) ^(0/40) ₅₃₀₋₇₅₀≤3%, an image generated by the imaging apparatus 100 is unlikely to be colored unevenly.

As shown in FIG. 2 , the imaging apparatus 100 further includes, for example, a color filter 3 that is disposed ahead of the imaging device 4 and is a filter of three colors, R (red), G (green), and B (blue). The optical filter 1 a is disposed ahead of the color filter 3. The color filter 3 and imaging device 4 receive light having been transmitted through the lens system 2. The light-absorbing layer 10 is, for example, arranged to be in contact with a side of the transparent dielectric substrate 20, the side being closer to the lens system 2. As described previously, the protecting effect on the lens system 2 or imaging device 4 increases when a hard material such as sapphire is used as the transparent dielectric substrate 20. For example, in the color filter 3, the three colors, R (red), G (green), and B (blue), are arranged in a matrix, and any one of the R (red), G (green), and B (blue) colors is disposed immediately above a sub-pixel of the imaging device 4. The imaging device 4 receives light coming from an object and having been transmitted through the lens system 2, optical filter 1 a, and color filter 3. The imaging apparatus 100 generates an image based on information on electric charge produced by the light received by the imaging device 4. The color filter 3 and imaging device 4 may be combined to configure a color image sensor.

The imaging apparatus 100 may be modified so that the optical filter 1 a will be disposed adjacent to the color filter 3. The imaging apparatus 100 may also be modified to include at least one of the optical filters 1 b to 1 e instead of the optical filter 1 a or in addition to the optical filter 1 a.

EXAMPLES

The present invention will be described in more detail by examples. The present invention is not limited to the examples given below.

Measurement of Transmittance Spectra

Transmittance spectra shown upon incidence of light with wavelengths of 300 to 1200 nm on optical filters according to Examples and Comparative Examples, intermediate products of some of the optical filters according to Examples and Comparative Examples, and laminates according to Reference Examples were measured using an ultraviolet-visible spectrophotometer (manufactured by JASCO Corporation, product name: V-670). In the transmittance spectrum measurement, the incident angle of incident light was set to at least any one of 0°, 30°, 35°, 40°, 45°, 50°, 55°, 60°, and 65°. From the results of the measurement of the transmittance spectrum shown by each of the optical filters according to Examples and Comparative Examples at each incident angle, a spectral transmittance curve (normalized spectral transmittance curve) normalized so that the maximum of the spectral transmittance in the wavelength range of 400 to 650 nm would be 100% was obtained for each incident angle. Based on the normalized spectral transmittance curves for the incident angles, an average ΔT_(S) ^(x/y) _(W-V) of absolute values of differences each between a value of a normalized spectral transmittance for the incident angle x° and a value of a normalized spectral transmittance for the incident angle y° in the wavelength range of W nm to V nm (W<V) was calculated.

Example 1

1.125 g of copper acetate monohydrate ((CH₃COO)₂Cu.H₂O) and 60 g of tetrahydrofuran (THF) were mixed and stirred for 3 hours to obtain a copper acetate solution. To the obtained copper acetate solution was then added 0.412 g of PLYSURF A208N (manufactured by DKS Co., Ltd.) which is a phosphoric acid ester compound, followed by stirring for 30 minutes to obtain a solution A. 10 g of THF was added to 0.176 g of phenylphosphonic acid (C₆H₅PO(OH)₂) (manufactured by Nissan Chemical Industries, Ltd.), followed by stirring for 30 minutes to obtain a solution B1-1. 10 g of THF was added to 1.058 g of 4-bromophenylphosphonic acid (C₆H₄BrPO(OH)₂) (manufactured by Tokyo Chemical Industry Co., Ltd.), followed by stirring for 30 minutes to obtain a solution B1-2. Next, the solutions B1-1 and B1-2 were mixed and stirred for 1 minute. 2.166 g of methyltriethoxysilane (MTES: CH₃Si(OC₂H₅)₃) (manufactured by Shin-Etsu Chemical Co., Ltd.) and 0.710 g of tetraethoxysilane (TEOS: Si(OC₂H₅)₄) (manufactured by KISHIDA CHEMICAL Co., Ltd., special grade) were added, and the mixture was further stirred for 1 minute to obtain a solution B1. The solution B1 was added to the solution A while the solution A was stirred, and the mixture was stirred at room temperature for 1 minute. To the resultant solution was then added 25 g of toluene, followed by stirring at room temperature for 1 minute to obtain a solution C1. The solution C1 was placed in a flask and subjected to solvent removal using a rotary evaporator (manufactured by Tokyo Rikakikai Co., Ltd., product code: N-1110SF) under heating by means of an oil bath (manufactured by Tokyo Rikakikai Co., Ltd., product code: OSB-2100). The temperature of the oil bath was controlled to 105° C. The solution having undergone the solvent removal was then collected from the flask. A solution D1 was thus obtained. The solution D1 was a dispersion of fine particles of copper phenyl-based phosphonate (light absorber) including copper phenylphosphonate and copper 4-bromophenylphosphonate. The solution D1 was transparent, and the fine particles of the light absorber were well dispersed therein.

1.125 g of copper acetate monohydrate and 36 g of THF were mixed and stirred for 3 hours to obtain a copper acetate solution. To the obtained copper acetate solution was then added 0.643 g of PLYSURF A208N which is a phosphoric acid ester compound, followed by stirring for 30 minutes to obtain a solution E1. 10 g of THF was added to 0.722 g of n-butylphosphonic acid (C₄H₉PO(OH)₂) (manufactured by Nippon Chemical Industrial Co., Ltd.), followed by stirring for 30 minutes to obtain a solution F1. The solution F1 was added to the solution E1 while the solution E1 was stirred, and the mixture was stirred at room temperature for 1 minute. To the resultant solution was then added 25 g of toluene, followed by stirring at room temperature for 1 minute to obtain a solution G1. The solution G1 was placed in a flask and subjected to solvent removal using a rotary evaporator under heating by means of an oil bath. The temperature of the oil bath was controlled to 105° C. The solution having undergone the solvent removal was then collected from the flask. A solution H1 was thus obtained. The solution H1 was a dispersion of fine particles of copper butylphosphonate. The solution H1 was transparent, and the fine particles were well dispersed therein.

To the solution D1 was added 2.200 g of a silicone resin (manufactured by Shin-Etsu Chemical Co., Ltd., product name: KR-300), followed by stirring for 30 minutes to obtain a solution I1. The solution H1 was added to the solution I1, followed by stirring for 30 minutes to obtain a light-absorbing composition according to Example 1.

The light-absorbing composition according to Example 1 was applied with a dispenser to a 30 mm×30 mm central region of each surface of a transparent glass substrate (manufactured by SCHOTT AG, product name: D 263 T eco) made of borosilicate glass and having dimensions of 76 mm×76 mm×0.07 mm. Films were thus formed on the substrate. When the light-absorbing composition was applied to the transparent glass substrate, a frame having an opening corresponding in dimensions to the region where the film-forming liquid was applied was put on the transparent glass substrate to hold back the film-forming liquid and prevent the film-forming liquid from spreading. After the application to one surface of the transparent glass substrate, the transparent glass substrate was left at ordinary temperature until the applied light-absorbing composition lost its flowability. Then, the light-absorbing composition was applied also to the other surface of the transparent glass substrate in the same manner. The amount of the light-absorbing composition applied was determined so that the sum of the thicknesses of the layers which were originally the light-absorbing composition films and were formed on both surfaces of the transparent glass substrate would eventually be about 180 μm. Subsequently, the transparent glass substrate with the undried light-absorbing composition films was placed in an oven and heat-treated at 85° C. for 6 hours to cure the film. After that, the transparent glass substrate with the films formed thereon was placed in a thermo-hygrostat set at a temperature of 85° C. and a relative humidity of 85% for a 20-hour humidification treatment. The humidification treatment was performed to promote hydrolysis and polycondensation of the alkoxysilane monomer contained in the light-absorbing composition applied onto the transparent glass substrate and form a hard and dense matrix of each light-absorbing layer. After that, a region with the light-absorbing layers formed on the transparent glass substrate was cut out to obtain an optical filter according to Example 1. The sum of the thicknesses of the light-absorbing layers on both surfaces of the optical filter according to Example 1 is 183 μm. Transmittance spectra shown by the optical filter according to Example 1 at incident angles of 0°, 30°, 35°, 40°, 45°, 50°, 55°, 60°, and 65° are shown in FIGS. 3A and 3B. Values of characteristics derived from the transmittance spectrum shown by the optical filter according to Example 1 at an incident angle of 0° are shown in Table 3. Normalized spectral transmittance curves shown by the optical filter according to Example 1 at incident angles of 0°, 30°, 35°, 40°, 45°, 50°, 55°, 60°, and 65° are shown in FIGS. 4A and 4B. Values of ΔT_(S) ⁰/y_(W-V) of the optical filter according to Example 1 for an incident angle x° of 0° and values of ΔT_(S) ³⁰/y_(W-V) of the optical filter according to Example 1 for an incident angle x° of 30° are shown in Tables 4 and 5, respectively.

As shown in Table 3, the above requirements (1) to (9) are satisfied by the optical filter according to Example 1. As shown in Tables 4 and 5, the values of ΔT_(S) ⁰/y_(W-V) and ΔT_(S) ³⁰/y_(W-V) of the optical filter according to Example 1 satisfy the requirements shown in Tables 1 and 2, respectively. For the optical filter according to Example 1, as shown in FIGS. 3A and 3B, the transmittances in a wavelength region of 380 nm or less and a wavelength region of 700 nm or more are sufficiently low, and the transmittances at a wavelength of 450 nm and in the wavelength range of 500 to 600 nm are sufficiently high. In other words, the optical filter according to Example 1 can favorably block light in the ultraviolet and near-infrared regions and has characteristics of allowing light in the visible region to be transmitted sufficiently. For the optical filter according to Example 1, as shown in FIGS. 4A and 4B, the normalized spectral transmittances for incident angles of 0° to 65° are sufficiently low in a wavelength region of 380 nm or less and a wavelength region of 700 nm or more, and the normalized spectral transmittances for incident angles of 0° to 65° are sufficiently high at a wavelength of 450 nm and in the wavelength range of 500 to 600 nm. Therefore, the optical filter according to Example 1 favorably blocks light in the ultraviolet and near-infrared regions and has advantageous characteristics for sufficiently transmitting light in the visible region, even when sensitivity correction is made so as to cover a decrease in the amount of light in accordance with the angle of light assumed from a design viewpoint to be incident on an imaging device in an imaging apparatus. Additionally, each gap between the shapes of one and another of the normalized spectral transmittance curves shown by the optical filter according to Example 1 at the incident angles is small, and an image generated by an imaging apparatus employing the optical filter according to Example 1 is deemed to be unlikely to be colored unevenly.

Example 2

1.125 g of copper acetate monohydrate ((CH₃COO)₂Cu.H₂O) and 60 g of tetrahydrofuran (THF) were mixed and stirred for 3 hours to obtain a copper acetate solution. To the obtained copper acetate solution was then added 0.412 g of PLYSURF A208N (manufactured by DKS Co., Ltd.) which is a phosphoric acid ester compound, followed by stirring for 30 minutes to obtain a solution A. 10 g of THF was added to 0.441 g of phenylphosphonic acid (C₆H₅PO(OH)₂) (manufactured by Nissan Chemical Industries, Ltd.), followed by stirring for 30 minutes to obtain a solution B2-1. 10 g of THF was added to 0.661 g of 4-bromophenylphosphonic acid (C₆H₄BrPO(OH)₂) (manufactured by Tokyo Chemical Industry Co., Ltd.), followed by stirring for 30 minutes to obtain a solution B2-2. Next, the solutions B2-1 and B2-2 were mixed and stirred for 1 minute. 1.934 g of methyltriethoxysilane (MTES: CH₃Si(OC₂H₅)₃) (manufactured by Shin-Etsu Chemical Co., Ltd.) and 0.634 g of tetraethoxysilane (TEOS: Si(OC₂H₅)₄) (manufactured by KISHIDA CHEMICAL Co., Ltd., special grade) were added, and the mixture was further stirred for 1 minute to obtain a solution B2. The solution B2 was added to the solution A while the solution A was stirred, and the mixture was stirred at room temperature for 1 minute. To the resultant solution was then added 25 g of toluene, followed by stirring at room temperature for 1 minute to obtain a solution C2. The solution C2 was placed in a flask and subjected to solvent removal using a rotary evaporator (manufactured by Tokyo Rikakikai Co., Ltd., product code: N-1110SF) under heating by means of an oil bath (manufactured by Tokyo Rikakikai Co., Ltd., product code: OSB-2100). The temperature of the oil bath was controlled to 105° C. The solution having undergone the solvent removal was then collected from the flask. A solution D2 was thus obtained. The solution D2 was a dispersion of fine particles of copper phenyl-based phosphonate (light absorber) including copper phenylphosphonate and copper 4-bromophenylphosphonate. The solution D2 was transparent, and the fine particles were well dispersed therein.

1.125 g of copper acetate monohydrate and 36 g of THF were mixed and stirred for 3 hours to obtain a copper acetate solution. To the obtained copper acetate solution was then added 0.710 g of PLYSURF A208N which is a phosphoric acid ester compound, followed by stirring for 30 minutes to obtain a solution E2. 10 g of THF was added to 0.708 g of n-butylphosphonic acid (C₄H₉PO(OH)₂) (manufactured by Nippon Chemical Industrial Co., Ltd.), followed by stirring for 30 minutes to obtain a solution F2. The solution F2 was added to the solution E2 while the solution E2 was stirred, and the mixture was stirred at room temperature for 1 minute. To the resultant solution was then added 25 g of toluene, followed by stirring at room temperature for 1 minute to obtain a solution G2. This solution G2 was placed in a flask and subjected to solvent removal using a rotary evaporator under heating by means of an oil bath. The temperature of the oil bath was controlled to 105° C. The solution having undergone the solvent removal was then collected from the flask. A solution H2 was thus obtained. The solution H2 was a dispersion of fine particles of copper butylphosphonate. The solution H2 was transparent, and the fine particles were well dispersed therein.

To the solution D2 was added 2.200 g of a silicone resin (manufactured by Shin-Etsu Chemical Co., Ltd., product name: KR-300), followed by stirring for 30 minutes to obtain a solution I2. The solution H2 was added to the solution I2, followed by stirring for 30 minutes to obtain a light-absorbing composition according to Example 2.

The light-absorbing composition according to Example 2 was applied with a dispenser to a 30 mm×30 mm central region of one principal surface of a transparent glass substrate (manufactured by SCHOTT AG, product name: D 263 T eco) made of borosilicate glass and having dimensions of 76 mm×76 mm×0.21 mm. A film was thus formed on the substrate. When the light-absorbing composition was applied to the transparent glass substrate, a frame having an opening corresponding in dimensions to the region where the film-forming liquid was applied was put on the transparent glass substrate to hold back the film-forming liquid and prevent the film-forming liquid from spreading. The amount of the light-absorbing composition applied was determined so that the thickness of the layer which was originally the light-absorbing composition film would eventually be about 170 μm. Subsequently, the transparent glass substrate with the undried light-absorbing composition film was placed in an oven and heat-treated at 85° C. for 6 hours to cure the film. After that, the transparent glass substrate with the film formed thereon was placed in a thermo-hygrostat set at a temperature of 85° C. and a relative humidity of 85% for a 20-hour humidification treatment. An optical filter according to Example 2 including a light-absorbing layer formed on a transparent glass substrate was thus obtained. The humidification treatment was performed to promote hydrolysis and polycondensation of the alkoxysilane monomer contained in the light-absorbing composition applied onto the transparent glass substrate and form a hard and dense matrix of the light-absorbing layer. After that, a region with the light-absorbing layer formed on a transparent glass substrate was cut out to obtain the optical filter according to Example 2. The thickness of the light-absorbing layer of the optical filter according to Example 2 is 170 μm. Transmittance spectra shown by the optical filter according to Example 2 at incident angles of 0°, 30°, 35°, 40°, 45°, 50°, 55°, 60°, and 65° are shown in FIGS. 5A and 5B. Values of characteristics derived from the transmittance spectrum shown by the optical filter according to Example 2 at an incident angle of 0° are shown in Table 6. Normalized spectral transmittance curves shown by the optical filter according to Example 2 at incident angles of 0°, 30°, 35°, 4°, 45°, 50°, 55°, 60°, and 65° are shown in FIGS. 6A and 6B. Values of ΔT_(S) ⁰/y_(W-V) of the optical filter according to Example 2 for an incident angle x° of 0° and values of ΔT_(S) ³⁰/y_(W-V) of the optical filter according to Example 2 for an incident angle x° of 30° are shown in Table 7 and Table 8, respectively.

As shown in Table 6, the above requirements (1) to (9) are satisfied by the optical filter according to Example 2. As shown in Tables 7 and 8, the values of ΔT_(S) ⁰/y_(W-V) and ΔT_(S) ³⁰/y_(W-V) of the optical filter according to Example 2 satisfy the requirements shown in Tables 1 and 2, respectively. As shown in FIGS. 5A and 5B, the optical filter according to Example 2 has transmission bands extending to a short wavelength side compared to the transmission bands of the optical filter according to Example 1, and has transmittances slightly less than 20% at a wavelength of 380 nm. According to Japanese Industrial Standards (JIS) Z 8120, the short-wavelength limit in the wavelength range of an electromagnetic wave equivalent to a visible ray is 360 to 400 nm. It can be said that the transmittance of the optical filter according to Example 2 sharply increases around the short-wavelength limit of a visible ray with increase in wavelength. For the optical filter according to Example 2, transmission of a small amount of light was observed in a band of more than 1100 nm. In this band, however, common imaging devices have a low sensitivity. Therefore, incorporating the optical filter according to Example 2 in an imaging apparatus is not considered problematic in practical use.

For the optical filter according to Example 2, the transmittances in a wavelength region of less than 380 nm and a wavelength region of 700 nm or more, exclusive of a wavelength region of 1100 nm or more, are sufficiently low and the transmittances at a wavelength of 450 nm and in the wavelength range of 500 to 600 nm are sufficiently high. The optical filter according to Example 2 can favorably block light in the ultraviolet and near-infrared regions and has characteristics of allowing light in the visible region to be transmitted sufficiently. For the optical filter according to Example 2, as shown in FIGS. 6A and 6B, the normalized spectral transmittances for incident angles of 0° to 65° are sufficiently low in a wavelength region of less than 380 nm and a wavelength region of 700 nm or more exclusive of a wavelength region of 1100 nm or more, and the normalized spectral transmittances for incident angles of 0° to 65° are sufficiently high at a wavelength of 450 nm and in the wavelength range of 500 to 600 nm. Therefore, the optical filter according to Example 2 favorably blocks light in the ultraviolet and near-infrared regions and has advantageous characteristics for sufficiently transmitting light in the visible region, even when sensitivity correction is made so as to cover a decrease in the amount of light in accordance with the angle of light assumed from a design viewpoint to be incident on an imaging device in an imaging apparatus. Additionally, each gap between the shapes of one and another of the normalized spectral transmittance curves shown by the optical filter according to Example 2 at the incident angles is small, and an image generated by an imaging apparatus employing the optical filter according to Example 2 is deemed to be unlikely to be colored unevenly. The optical filter according to Example 2 includes the light-absorbing layer only on one surface of the transparent glass substrate. Therefore, in order to reduce warping of the transparent glass substrate due to stress in the light-absorbing layer, the transparent glass substrate is thicker than the transparent glass substrate of the optical filter according to Example 1. In other words, the thickness of a transparent glass substrate is easily reduced by formation of a light-absorbing layer on each surface of the transparent glass substrate, as in the optical filter according to Example 1.

Example 3

1.125 g of copper acetate monohydrate ((CH₃COO)₂Cu.H₂O) and 60 g of tetrahydrofuran (THF) were mixed and stirred for 3 hours to obtain a copper acetate solution. To the obtained copper acetate solution was then added 0.412 g of PLYSURF A208N (manufactured by DKS Co., Ltd.) which is a phosphoric acid ester compound, followed by stirring for 30 minutes to obtain a solution A. 10 g of THF was added to 0.176 g of phenylphosphonic acid (C₆H₅PO(OH)₂) (manufactured by Nissan Chemical Industries, Ltd.), followed by stirring for 30 minutes to obtain a solution B3-1. 10 g of THF was added to 1.058 g of 4-bromophenylphosphonic acid (C₆H₄BrPO(OH)₂) (manufactured by Tokyo Chemical Industry Co., Ltd.), followed by stirring for 30 minutes to obtain a solution B3-2. Next, the solutions B3-1 and B3-2 were mixed and stirred for 1 minute. 2.166 g of methyltriethoxysilane (MTES: CH₃Si(OC₂H₅)₃) (manufactured by Shin-Etsu Chemical Co., Ltd.) and 0.710 g of tetraethoxysilane (TEOS: Si(OC₂H₅)₄) (manufactured by KISHIDA CHEMICAL Co., Ltd., special grade) were added, and the mixture was further stirred for 1 minute to obtain a solution B3. The solution B3 was added to the solution A while the solution A was stirred, and the mixture was stirred at room temperature for 1 minute. To the resultant solution was then added 25 g of toluene, followed by stirring at room temperature for 1 minute to obtain a solution C3. This solution C3 was placed in a flask and subjected to solvent removal using a rotary evaporator (manufactured by Tokyo Rikakikai Co., Ltd., product code: N-1110SF) under heating by means of an oil bath (manufactured by Tokyo Rikakikai Co., Ltd., product code: OSB-2100). The temperature of the oil bath was controlled to 105° C. The solution having undergone the solvent removal was then collected from the flask. A solution D3 was thus obtained. The solution D3 was a dispersion of fine particles of copper phenyl-based phosphonate (light absorber) including copper phenylphosphonate and copper 4-bromophenylphosphonate. The solution D3 was transparent, and the fine particles were well dispersed therein.

1.125 g of copper acetate monohydrate and 36 g of THF were mixed and stirred for 3 hours to obtain a copper acetate solution. To the obtained copper acetate solution was then added 0.643 g of PLYSURF A208N which is a phosphoric acid ester compound, followed by stirring for 30 minutes to obtain a solution E3. 10 g of THF was added to 0.722 g of n-butylphosphonic acid (C₄H₉PO(OH)₂) (manufactured by Nippon Chemical Industrial Co., Ltd.), followed by stirring for 30 minutes to obtain a solution F3. The solution F3 was added to the solution E3 while the solution E3 was stirred, and the mixture was stirred at room temperature for 1 minute. To the resultant solution was then added 25 g of toluene, followed by stirring at room temperature for 1 minute to obtain a solution G3. This solution G3 was placed in a flask and subjected to solvent removal using a rotary evaporator under heating by means of an oil bath. The temperature of the oil bath was controlled to 105° C. The solution having undergone the solvent removal was then collected from the flask. A solution H3 was thus obtained. The solution H3 was a dispersion of fine particles of copper butylphosphonate. The solution H3 was transparent, and the fine particles were well dispersed therein.

To the solution D3 was added 2.200 g of a silicone resin (manufactured by Shin-Etsu Chemical Co., Ltd., product name: KR-300), followed by stirring for 30 minutes to obtain a solution I3. The solution H3 was added to the solution I3, followed by stirring for 30 minutes to obtain a light-absorbing composition according to Example 3.

The light-absorbing composition according to Example 3 was applied with a dispenser to a 30 mm×30 mm central region of one surface of a transparent glass substrate (manufactured by SCHOTT AG, product name: D 263 T eco) made of borosilicate glass and having dimensions of 76 mm×76 mm×0.21 mm. A film was thus formed on the substrate. When the light-absorbing composition was applied to the transparent glass substrate, a frame having an opening corresponding in dimensions to the region where the film-forming liquid was applied was put on the transparent glass substrate to hold back the film-forming liquid and prevent the film-forming liquid from spreading. The amount of the light-absorbing composition applied was determined so that the thickness of the layer which was originally the light-absorbing composition film would eventually be about 135 μm. Subsequently, the transparent glass substrate with the undried film was placed in an oven and heat-treated at 85° C. for 6 hours to cure the film. After that, the transparent glass substrate with the film formed thereon was placed in a thermo-hygrostat set at a temperature of 85° C. and a relative humidity of 85% for a 20-hour humidification treatment to form a light-absorbing layer on the transparent glass substrate. The humidification treatment was performed to promote hydrolysis and polycondensation of the alkoxysilane monomer contained in the light-absorbing composition applied onto the transparent glass substrate and form a hard and dense matrix of the light-absorbing layer. The light-absorbing layer on the transparent glass substrate thus obtained was peeled off to obtain an optical filter according to Example 3. The thickness of the optical filter according to Example 3 is 135 μm. Transmittance spectra shown by the optical filter according to Example 3 at incident angles of 0°, 30°, 35°, 40°, 45°, 50°, 5°, 60°, and 65° are shown in FIGS. 7A and 7B. Values of characteristics derived from the transmittance spectrum shown by the optical filter according to Example 3 at an incident angle of 0° are shown in Table 9. Normalized spectral transmittance curves shown by the optical filter according to Example 3 at incident angles of 0°, 30°, 35°, 40°, 45°, 50°, 5°, 60°, and 65° are shown in FIGS. 8A and 8B. Values of ΔT_(S) ⁰/y_(W-V) of the optical filter according to Example 3 for an incident angle x° of 0° and values of ΔT_(S) ³⁰/y_(W-V) of the optical filter according to Example 3 for an incident angle x° of 30° are shown in Tables 10 and 11, respectively.

As shown in Table 9, the above requirements (1) to (9) are satisfied by the optical filter according to Example 3. As shown in Tables 10 and 11, the values of ΔT_(S) ⁰/y_(W-V) and ΔT_(S) ³⁰/y_(W-V) of the optical filter according to Example 3 satisfy the requirements shown in Tables 1 and 2, respectively. For the optical filter according to Example 3, the transmittances at wavelengths of 700 nm and 715 nm are within the acceptable range, albeit slightly high compared to those for the optical filters according to Examples 1 and 2. For the optical filter according to Example 3, transmission of a small amount of light was observed in a band of more than 1100 nm unlike in the case of the optical filter according to Example 1, but the transmittance of light in this band was suppressed compared to the case of the optical filter according to Example 2. In this band, common imaging devices have a low sensitivity. Therefore, incorporating the optical filter according to Example 3 in an imaging apparatus is not considered problematic in practical use. For the optical filter according to Example 3, the transmittances in a wavelength region of 380 nm or less are sufficiently low, and the transmittances at a wavelength of 450 nm and in the wavelength region of 500 to 600 nm are sufficiently high. In other words, the optical filter according to Example 3 can favorably block light in the ultraviolet and near-infrared regions and has characteristics of allowing light in the visible region to be transmitted sufficiently.

For the optical filter according to Example 3, as shown in FIGS. 8A and 8B, the normalized spectral transmittances for incident angles of 0° to 65° are sufficiently low in a wavelength region of 380 nm or less and a wavelength region of 700 nm or more, and the normalized spectral transmittances for incident angles of 0° to 65° are sufficiently high at a wavelength of 450 nm and in the wavelength range of 500 to 600 nm. Therefore, the optical filter according to Example 3 favorably blocks light in the ultraviolet and near-infrared regions and has advantageous characteristics for sufficiently transmitting light in the visible region, even when sensitivity correction is made so as to cover a decrease in the amount of light in accordance with the angle of light assumed from a design viewpoint to be incident on an imaging device in an imaging apparatus. Additionally, each gap between the shapes of one and another of the normalized spectral transmittance curves shown by the optical filter according to Example 3 at the incident angles is small, and an image generated by an imaging apparatus employing the optical filter according to Example 3 is deemed to be unlikely to be colored unevenly. Since the optical filter according to Example 3 does not include a transparent glass substrate and is composed only of a light-absorbing layer, the thickness of the optical filter can be reduced.

Example 4

1.1 g of copper acetate monohydrate and 60 g of tetrahydrofuran (THF) were mixed and stirred for 3 hours. To the obtained solution was added 2.3 g of a phosphoric acid ester (manufactured by DKS Co., Ltd., product name: PLYSURF A208F), followed by stirring for 30 minutes to obtain a solution A4. 10 g of THF was added to 0.6 g of phenylphosphonic acid (manufactured by Tokyo Chemical Industry Co., Ltd.), followed by stirring for 30 minutes to obtain a solution B4. The solution B4 was added to the solution A4 while the solution A4 was stirred, and the mixture was stirred at room temperature for 1 minute. To the resultant solution was added 45 g of toluene, followed by stirring at room temperature for 1 minute to obtain a solution C4. The solution C4 was placed in a flask and subjected to solvent removal for 25 minutes using a rotary evaporator (manufactured by Tokyo Rikakikai Co., Ltd., product code: N-1110SF) under heating by means of an oil bath (manufactured by Tokyo Rikakikai Co., Ltd., product code: OSB-2100) controlled to 120° C. The solution having undergone the solvent removal was taken out of the flask, and to the solution was added 4.4 g of a silicone resin (manufactured by Shin-Etsu Chemical Co., Ltd., product name: KR-300), followed by stirring at room temperature for 30 minutes to obtain a light-absorbing composition IRA1.

2.25 g of copper acetate monohydrate and 120 g of tetrahydrofuran (THF) were mixed and stirred for 3 hours. To the obtained solution was added 1.8 g of a phosphoric acid ester (manufactured by DKS Co., Ltd., product name: PLYSURF A208F), followed by stirring for 30 minutes to obtain a solution E4. 20 g of THF was added to 1.35 g of butylphosphonic acid, followed by stirring for 30 minutes to obtain a solution F4. The solution F4 was added to the solution E4 while the solution E4 was stirred, and the mixture was stirred at room temperature for 3 hours. To the resultant solution was added 40 g of toluene, and the solvent was evaporated in an 85° C. environment over 7.5 hours. To the resultant solution was added 8.8 g of a silicone resin (manufactured by Shin-Etsu Chemical Co., Ltd., product name: KR-300), followed by stirring for 3 hours to obtain a light-absorbing composition IRA2.

The light-absorbing composition IRA1 obtained was applied to one principal surface of a transparent glass substrate (manufactured by SCHOTT AG, product name: D 263 T eco) using a die coater. The resultant film was cured by heat treatment in an oven at 85° C. for 3 hours, at 125° C. for 3 hours, at 150° C. for 1 hour, and then at 170° C. for 3 hours to form a light-absorbing layer frail. The light-absorbing composition IRA1 was applied in the same manner to the other principal surface of the transparent glass substrate. The resultant film was cured under the same conditions as the conditions for forming the light-absorbing layer ira11 to form a light-absorbing layer ira12. The total thickness of the light-absorbing layer frail and light-absorbing layer ira12 is 0.2 mm. An intermediate product a was thus obtained. A transmittance spectrum obtained upon incidence of light with a wavelength of 300 to 1200 nm on the intermediate product a at an incident angle of 0° is shown in FIG. 9A. In this transmittance spectrum, the spectral transmittance at a wavelength of 380 nm is 10.9%, the spectral transmittance at a wavelength of 450 nm is 85.7%, the average of the spectral transmittance in the wavelength range of 500 to 600 nm is 88.1%, the spectral transmittance at a wavelength of 700 nm is 2.3%, the spectral transmittance at a wavelength of 715 nm is 0.9%, the average of the spectral transmittance in the wavelength range of 700 to 800 nm is 0.4%, the maximum of the spectral transmittance in the wavelength range of 750 to 1080 nm is 7.6%, and the maximum of the spectral transmittance in the wavelength range of 1000 to 1100 nm is 12.1%.

A 500-nm-thick SiO₂ film was vapor-deposited on the light-absorbing layer frail and light-absorbing layer ira12 using a vacuum deposition apparatus to form a protective layer p1 and protective layer p2, respectively. The light-absorbing composition IRA2 was applied onto the surface of the protective layer p1 with a die coater. The resultant film was cured by heat treatment in an oven at 85° C. for 3 hours, at 125° C. for 3 hours, at 150° C. for 1 hour, and then at 170° C. for 3 hours to form a light-absorbing layer ira21. The light-absorbing composition IRA2 was applied also onto the protective layer p2. The resultant film was cured under the same heating conditions as the conditions for forming the light-absorbing layer ira21 to form a light-absorbing layer ira22. The total thickness of the light-absorbing layer ira21 and light-absorbing layer ira22 is 50 μm. An intermediate product 13 was thus obtained. A transmittance spectrum obtained upon incidence of light with a wavelength of 300 to 1200 nm on the intermediate product 13 at an incident angle of 0° is shown in FIG. 9B. In this transmittance spectrum, the spectral transmittance at a wavelength of 380 nm is 10.5%, the spectral transmittance at a wavelength of 450 nm is 84.0%, the average of the spectral transmittance in the wavelength range of 500 to 600 nm is 87.2%, the spectral transmittance at a wavelength of 700 nm is 1.8%, the spectral transmittance at a wavelength of 715 nm is 0.6%, the average of the spectral transmittance in the wavelength range of 700 to 800 nm is 0.3%, the maximum of the spectral transmittance in the wavelength range of 750 to 1080 nm is 0.7%, and the maximum of the spectral transmittance in the wavelength range of 1000 to 1100 nm is 1.2%.

A 500-nm-thick SiO₂ film was vapor-deposited on the infrared-absorbing layer ira22 using a vacuum deposition apparatus to form a protective layer p3.

To a solution containing MEK as a solvent and an ultraviolet-absorbing substance composed of a benzophenone-based ultraviolet-absorbing substance which has low light absorption in the visible region and is soluble in methyl ethyl ketone (MEK) was added polyvinyl butyral (PVB) in an amount equivalent to 60 weight % of the solids of the solution, followed by stirring for 2 hours to obtain a light-absorbing composition UVA1.

The light-absorbing composition UVA1 was applied onto the protective layer p3 by spin coating, followed by curing of the resultant film by heating at 140° C. for 30 minutes to form a light-absorbing layer uva1. The thickness of the light-absorbing layer uva1 is 6 μm. Separately, a 6-μm-thick light-absorbing layer uva1 was formed on one principal surface of a transparent glass substrate (manufactured by SCHOTT AG, product name: D 263 T eco) using the light-absorbing composition UVA1 to obtain a laminate according to Reference Example 1. A transmittance spectrum obtained upon incidence of light with a wavelength of 300 to 1200 nm on the laminate according to Reference Example 1 at an incident angle of 0° is shown in FIG. 9C.

An anti-reflection film ar1 and anti-reflection film ar2 were formed on the light-absorbing layer ira21 and light-absorbing layer uva1, respectively, by vacuum deposition. The specifications of the anti-reflection film ar1 and anti-reflection film ar2 were the same. Each of the anti-reflection film ar1 and anti-reflection film ar2 was a film composed of SiO₂ and TiO₂ that were alternately laminated. Each of the anti-reflection film ar1 and anti-reflection film ar2 included seven layers and had a total thickness of about 0.4 μm. An optical filter according to Example 4 was thus obtained. Additionally, an anti-reflection film an was formed on one surface of a transparent glass substrate (manufactured by SCHOTT AG, product name: D 263 T eco) to obtain a laminate according to Reference Example 2. Transmittance spectra obtained upon incidence of light with a wavelength of 300 to 1200 nm on the laminate according to Reference Example 2 at incident angles of 0°, 30°, 50° and 65° are shown in FIG. 9D. For the laminate according to Reference Example 2, as shown in FIG. 9D, a wavelength band including a local transmittance decrease does not exist in the wavelength range of 400 to 700 nm for any of the incident angles.

Transmittance spectra shown by the optical filter according to Example 4 at incident angles of 0°, 30°, 35°, 40°, 45°, 50°, 55°, 60°, and 65° are shown in FIGS. 10A and 10B. Values of characteristics derived from the transmittance spectrum shown by the optical filter according to Example 4 at an incident angle of 0° are shown in Table 12. Normalized spectral transmittance curves shown by the optical filter according to Example 4 at incident angles of 0°, 30°, 35°, 40°, 45°, 50°, 55°, 60°, and 65° are shown in FIGS. 11A and 11B. Values of ΔT_(S) ⁰/y_(W-V) of the optical filter according to Example 4 for an incident angle x° of 0° and values of ΔT_(S) ³⁰/y_(W-V) of the optical filter according to Example 4 for an incident angle x° of 30° are shown in Tables 13 and 14, respectively.

As shown in Table 12, the above requirements (1) to (9) are satisfied by the optical filter according to Example 4. As shown in Tables 13 and 14, the values of ΔT_(S) ⁰/y_(W-V) and ΔT_(S) ³⁰/y_(W-V) of the optical filter according to Example 4 satisfy the requirements shown in Tables 1 and 2, respectively. For the optical filter according to Example 4, the transmittances in a wavelength region of 380 nm or less and a wavelength region of 700 nm or more are sufficiently low, and the transmittances at a wavelength of 450 nm and in the wavelength region of 500 to 600 nm are sufficiently high. In other words, the optical filter according to Example 4 can favorably block light in the ultraviolet and near-infrared regions and has characteristics of allowing light in the visible region to be transmitted sufficiently. Moreover, since the optical filter according to Example 4 includes the anti-reflection film, the optical filter according to Example 4 has high transmittances in the visible region compared to those of the optical filters according to Examples 1 to 3 in the visible region. Additionally, no ripple occurs in the wavelength range of 400 to 700 nm upon incidence of light on the optical filter according to Example 4 at incident angles of 0° to 65°. Furthermore, since the optical filter according to Example 4 includes the light-absorbing layer uva1, the transmittance sharply increases around 400 nm with increase in wavelength.

For the optical filter according to Example 4, as shown in FIGS. 11A and 11B, the normalized spectral transmittances for incident angles of 0° to 65° are sufficiently low in a wavelength region of 380 nm or less and a wavelength region of 700 nm or more, and the normalized spectral transmittances for incident angles of 0° to 65° are sufficiently high at a wavelength of 450 nm and in the wavelength range of 500 to 600 nm. Therefore, the optical filter according to Example 4 favorably blocks light in the ultraviolet and near-infrared regions and has advantageous characteristics for sufficiently transmitting light in the visible region, even when sensitivity correction is made so as to cover a decrease in the amount of light in accordance with the angle of light assumed from a design viewpoint to be incident on an imaging device in an imaging apparatus. Additionally, each gap between the shapes of one and another of the normalized spectral transmittance curves shown by the optical filter according to Example 4 at the incident angles is small, and an image generated by an imaging apparatus employing the optical filter according to Example 4 is deemed to be unlikely to be colored unevenly.

Comparative Example 1

A light-reflecting layer irr1 that reflects light with a wavelength in the range of 730 to 1100 nm was formed on one principal surface of a transparent glass substrate (manufactured by SCHOTT AG, product name: D 263 T eco) by alternately laminating SiO₂ and TiO₂ in 50 layers using a vacuum deposition apparatus. An intermediate product y was thus obtained. Transmittance spectra obtained upon incidence of light with a wavelength of 300 to 1200 nm on the intermediate product Y at incident angles of 0°, 30° and 50° are shown in FIG. 12A. In the transmittance spectrum for an incident angle of 0°, the spectral transmittance at a wavelength of 380 nm is less than 0.2%, the spectral transmittance at a wavelength of 450 nm is 94.8%, the average of the spectral transmittance in the wavelength range of 500 to 600 nm is 94.3%, the spectral transmittance at a wavelength of 700 nm is 62.8%, the spectral transmittance at a wavelength of 715 nm is 9.5%, the average of the spectral transmittance in the wavelength range of 700 to 800 nm is 6.1%, the maximum of the spectral transmittance in the wavelength range of 750 to 1080 nm is 1.0%, and the maximum of the spectral transmittance in the wavelength range of 1000 to 1100 nm is 0.5%. In the transmittance spectrum for an incident angle of 30°, the spectral transmittance at a wavelength of 380 nm is less than 0.2%, the spectral transmittance at a wavelength of 450 nm is 94.6%, the average of the spectral transmittance in the wavelength range of 500 to 600 nm is 93.3%, the spectral transmittance at a wavelength of 700 nm is 3.2%, the spectral transmittance at a wavelength of 715 nm is 1.4%, the average of the spectral transmittance in the wavelength range of 700 to 800 nm is 1.0%, the maximum of the spectral transmittance in the wavelength range of 750 to 1080 nm is 0.8%, and the maximum of the spectral transmittance in the wavelength range of 1000 to 1100 nm is 0.6%. In the transmittance spectrum for an incident angle of 50°, the spectral transmittance at a wavelength of 380 nm is 3.7%, the spectral transmittance at a wavelength of 450 nm is 84.0%, the average of the spectral transmittance in the wavelength range of 500 to 600 nm is 86.0%, the spectral transmittance at a wavelength of 700 nm is 1.6%, the spectral transmittance at a wavelength of 715 nm is 1.1%, the average of the spectral transmittance in the wavelength range of 700 to 800 nm is 0.9%, the maximum of the spectral transmittance in the wavelength range of 750 to 1080 nm is 6.8%, and the maximum of the spectral transmittance in the wavelength range of 1000 to 1100 nm is 12.7%.

A cyanine-based organic dye and squarylium-based organic dye which are soluble in MEK were added to MEK serving as a solvent to prepare a solution. PVB in an amount equivalent to 99 weight % of the solids of the solution was added to the solution, followed by stirring for 2 hours to obtain a coating liquid. This coating liquid was applied by spin coating onto a principal surface of the transparent glass substrate of the intermediate product y, the principal surface opposite to the principal surface on which the light-reflecting layer irr1 was formed, and the resultant film was cured by heating at 140° C. for 30 minutes to form a light-absorbing layer ira3. Separately, a light-absorbing layer ira3 was formed in the same manner on one principal surface of a transparent glass substrate (manufactured by SCHOTT AG, product name: D 263 T eco) to obtain a laminate according to Reference Example 3. A transmittance spectrum obtained upon incidence of light with a wavelength of 300 to 1200 nm on the laminate according to Reference Example 3 at an incident angle of 0° is shown in FIG. 12B. In this transmittance spectrum, the spectral transmittance at a wavelength of 380 nm is 80.1%, the spectral transmittance at a wavelength of 450 nm is 83.8%, the average of the spectral transmittance in the wavelength range of 500 to 600 nm is 86.9%, the spectral transmittance at a wavelength of 700 nm is 2.0%, the spectral transmittance at a wavelength of 715 nm is 2.6%, the average of the spectral transmittance in the wavelength range of 700 to 800 nm is 15.9%, the maximum of the spectral transmittance in the wavelength range of 750 to 1080 nm is 90.2%, and the maximum of the spectral transmittance in the wavelength range of 1000 to 1100 nm is 91.1%.

An anti-reflection film ar1 was formed on the light-absorbing layer ira3 by vacuum deposition according to the same specifications as those of the anti-reflection film ar1 of the optical filter according to Example 4. An optical filter according to Comparative Example 1 was fabricated in this manner.

Transmittance spectra shown by the optical filter according to Comparative Example 1 at incident angles of 0°, 30°, 35°, 40°, 45°, 50°, 55°, 60°, and 65° are shown in FIGS. 13A and 13B. Values of characteristics derived from the transmittance spectrum shown by the optical filter according to Comparative Example 1 at an incident angle of 0° are shown in Table 15. Normalized spectral transmittance curves shown by the optical filter according to Comparative Example 1 at incident angles of 0°, 30°, 35°, 40°, 45°, 50°, 55°, 60°, and 65° are shown in FIGS. 14A and 14B. Values of ΔT_(S) ⁰/y_(W-V) of the optical filter according to Comparative Example 1 for an incident angle x° of 0° and values of ΔT_(S) ³⁰/y_(W-V) of the optical filter according to Comparative Example 1 for an incident angle x° of 30° are shown in Tables 16 and 17, respectively.

As shown in Table 15, the optical filter according to Comparative Example 1 satisfies the above requirements (1) to (9). However, as shown in Table 16, the values of ΔT_(S) ⁰/y_(W-V) of the optical filter according to Comparative Example 1 do not satisfy the requirements shown in Table 1, except for ΔT_(S) ^(0/30) ₄₅₀₋₆₅₀, ΔT_(S) ^(0/30) ₅₃₀₋₇₅₀, and ΔT_(S) ^(0/35) ₄₅₀₋₆₅₀. As shown in Table 17, the values of ΔT_(S) ³⁰/y_(W-V) of the optical filter according to Comparative Example 1 do not satisfy the requirements shown in Table 2, except for ΔT_(S) ^(30/35) ₄₅₀₋₆₅₀, ΔT_(S) ^(30/35) ₆₅₀₋₁₂₀₀. As shown in Tables 13A and 13B, the influence of a shift of the reflection band of the light-reflecting layer irr1 to the short wavelength side grows with increase in incident angle of light incident on the optical filter according to Comparative Example 1. Additionally, a large ripple occurs around 500 nm. Therefore, many of the values of ΔT_(S) ⁰/y_(W-V) and ΔT_(S) ³⁰/y_(W-V) of the optical filter according to Comparative Example 1 greatly exceed the upper limits shown in Tables 1 and 2.

The optical filter according to Comparative Example 1 blocks light in the near-infrared region not only by the action of the light-absorbing layer but also by the action of the light-reflecting layer. The light-reflecting layer exhibits its function of reflecting light by an interference effect attributed to its multilayer film. Thus, incidence of light at a large incident angle larger than a design value results not only in a shift of a wavelength band of reflected light to the short wavelength side but also in a ripple in a wavelength band of light which should be transmitted and severe distortion of the resultant spectral transmittance curve. Therefore, although the transmittance spectrum of light vertically incident on the optical filter according to Comparative Example 1 satisfies the desired requirements, the transmittance spectra of light incident thereon at larger incident angles cannot satisfy the desired requirements. Therefore, when an imaging apparatus in which the optical filter according to Comparative Example 1 is incorporated is used to take an object at a wide angle of view, for example, for a wide-angle shot, it is difficult to reproduce an even color tone of the object in the image taken and there is also concern that the image obtained may be colored quite unevenly.

Comparative Example 2

A light-absorbing transparent substrate bg1 was prepared. A transmittance spectrum obtained upon incidence of light with a wavelength of 300 to 1200 nm on the light-absorbing transparent substrate bg1 at an incident angle of 0° is shown in FIG. 15A. In this transmittance spectrum, the spectral transmittance at a wavelength of 380 nm is 86.8%, the spectral transmittance at a wavelength of 450 nm is 90.2%, the average of the spectral transmittance in the wavelength range of 500 to 600 nm is 86.5%, the spectral transmittance at a wavelength of 700 nm is 29.8%, the spectral transmittance at a wavelength of 715 nm is 25.3%, the average of the spectral transmittance in the wavelength range of 700 to 800 nm is 19.1%, the maximum of the spectral transmittance in the wavelength range of 750 to 1080 nm is 30.2%, and the maximum of the spectral transmittance in the wavelength range of 1000 to 1100 nm is 32.5%.

A light-reflecting layer irr2 that reflects light in the wavelength range of 720 to 1100 nm were formed on one principal surface of the light-absorbing transparent substrate bg1 by alternately laminating SiO₂ and TiO₂ in 54 layers using a vacuum deposition apparatus. Separately, a light-reflecting layer irr2 was formed in the same manner on one principal surface of a transparent glass substrate (manufactured by SCHOTT AG, product name: D 263 T eco) to fabricate a laminate according to Reference Example 4. Transmittance spectra obtained upon incidence of light with a wavelength of 300 to 1200 nm on the laminate according to Reference Example 4 at incident angles of 0°, 30°, and 50° are shown in FIG. 15B. In the transmittance spectrum for an incident angle 0°, the spectral transmittance at a wavelength of 380 nm is less than 0.2%, the spectral transmittance at a wavelength of 450 nm is 94.3%, the average of the spectral transmittance in the wavelength range of 500 to 600 nm is 94.7%, the spectral transmittance at a wavelength of 700 nm is 73.5%, the spectral transmittance at a wavelength of 715 nm is 9.8%, the average of the spectral transmittance in the wavelength range of 700 to 800 nm is 6.7%, the maximum of the spectral transmittance in the wavelength range of 750 to 1080 nm is 0.7%, and the maximum of the spectral transmittance in the wavelength range of 1000 to 1100 nm is 0.3%. In the transmittance spectrum for an incident angle of 30°, the spectral transmittance at a wavelength of 380 nm is 1.6%, the spectral transmittance at a wavelength of 450 nm is 90.8%, the average transmittance in the wavelength range of 500 to 600 nm is 93.2%, the spectral transmittance at a wavelength of 700 nm is 2.7%, the spectral transmittance at a wavelength of 715 nm is 1.1%, the average of the spectral transmittance in the wavelength range of 700 to 800 nm is 0.8%, the maximum of the spectral transmittance in the wavelength range of 750 to 1080 nm is 0.7%, and the maximum of the spectral transmittance in the wavelength range of 1000 to 1100 nm is 1.0%. In the transmittance spectrum for an incident angle of 50°, the spectral transmittance at a wavelength of 380 nm is 49.4%, the spectral transmittance at a wavelength of 450 nm is 87.5%, the average of the spectral transmittance in the wavelength range of 500 to 600 nm is 89.8%, the spectral transmittance at a wavelength of 700 nm is 1.6%, the spectral transmittance at a wavelength of 715 nm is 0.8%, the average of the spectral transmittance in the wavelength range of 700 to 800 nm is 0.9%, the maximum of the spectral transmittance in the wavelength range of 750 to 1080 nm is 6.0%, and the maximum of the spectral transmittance in the wavelength range of 1000 to 1100 nm is 13.0%.

A benzophenone-based ultraviolet-absorbing substance having low light absorption in the visible region and soluble in MEK was used as an ultraviolet absorber, and an infrared-absorbing dye composed of a squarylium compound and cyanine compound was used as an infrared absorber. The ultraviolet absorber and infrared absorber were weighed and added to MEK serving as a solvent to prepare a solution. PVB in an amount equivalent to 99 weight % of the solids of the solution was added to the solution, followed by stirring for 2 hours to obtain a coating liquid. This coating liquid was applied to the other principal surface of the light-absorbing transparent substrate bg1 to form a light-absorbing layer uvira2. A light-absorbing layer uvira2 was formed in the same manner on one principal surface of a transparent glass substrate (manufactured by SCHOTT AG, product name: D 263 T eco) to obtain a laminate according to Reference Example 5. A transmittance spectrum shown upon incidence of light with a wavelength of 300 to 1200 nm on the laminate according to Reference Example 5 at an incident angle of 0° is shown in FIG. 15C. In this transmittance spectrum, the spectral transmittance at a wavelength of 380 nm is less than 0.2%, the spectral transmittance at a wavelength of 450 nm is 84.3%, the average of the spectral transmittance in the wavelength range of 500 to 600 nm is 88.7%, the spectral transmittance at a wavelength of 700 nm is 4.8%, the spectral transmittance at a wavelength of 715 nm is 8.4%, the average of the spectral transmittance in the wavelength range of 700 to 800 nm is 63.8%, the maximum of the spectral transmittance in the wavelength range of 750 to 1080 nm is 92.7%, and the maximum of the spectral transmittance in the wavelength range of 1000 to 1100 nm is 92.7%.

An anti-reflection film art was formed on the light-absorbing layer uvira2 formed on the other principal surface of the light-absorbing transparent substrate bg1 by vacuum deposition according to the same specifications as those of the anti-reflection film ar1 of the optical filter according to Example 4. An optical filter according to Comparative Example 2 was fabricated in this manner.

Transmittance spectra shown by the optical filter according to Comparative Example 2 at incident angles of 0°, 30°, 35°, 40°, 45°, 50°, 55°, 60°, and 65° are shown in FIGS. 16A and 16B. Values of characteristics derived from the transmittance spectrum shown by the optical filter according to Comparative Example 2 at an incident angle of 0° are shown in Table 18. Normalized spectral transmittance curves shown by the optical filter according to Comparative Example 2 at incident angles of 0°, 30°, 35°, 40°, 45°, 50°, 55°, 60°, and 65° are shown in FIGS. 17A and 17B. Values of ΔT_(S) ⁰/y_(W-V) of the optical filter according to Comparative Example 2 for an incident angle x° of 0° and values of ΔT_(S) ³⁰/y_(W-V) of the optical filter according to Comparative Example 2 for an incident angle x° of 30° are shown in Tables 19 and 20, respectively.

As shown in Table 18, the optical filter according to Comparative Example 2 satisfies the above requirements (1) to (9). However, as shown in Table 19, the values of ΔT_(S) ⁰/y_(W-V) of the optical filter according to Comparative Example 2 do not satisfy the requirements shown in Table 1, except for ΔT_(S) ^(0/30) ₃₈₀₋₅₃₀, ΔT_(S) ^(0/30) ₄₅₀₋₆₅₀, ΔT_(S) ^(0/30) ₅₃₀₋₇₅₀, ΔT_(S) ^(0/30) ₆₅₀₋₁₂₀₀, ΔT_(S) ^(0/30) ₃₈₀₋₁₂₀₀, ΔT_(S) ^(0/35) ₄₅₀₋₆₅₀, and ΔT_(S) ^(0/35) ₅₃₀₋₇₅₀. As shown in Table 20, the values of ΔT_(S) ³⁰/y_(W-V) of the optical filter according to Comparative Example 2 do not satisfy the requirements shown in Table 2, except for ΔT_(S) ^(30/35) ₃₈₀₋₅₃₀, ΔT_(S) ^(30/35) ₄₅₀₋₆₅₀, ΔT_(S) ^(30/35) ₅₃₀₋₇₅₀, ΔT_(S) ^(30/35) ₆₅₀₋₁₂₀₀, ΔT_(S) ^(30/35) ₃₈₀₋₁₂₀₀, and ΔT_(S) ^(30/35) ₅₃₀₋₇₅₀. As shown in Tables 16A and 16B, the influence of a shift of the reflection band of the light-reflecting layer irr2 to the short wavelength side grows with increase in incident angle of light incident on the optical filter according to Comparative Example 2. Additionally, a large ripple occurs around 500 nm. Therefore, many of the values of ΔT_(S) ⁰/y_(W-V) and ΔT_(S) ³⁰/y_(W-V) of the optical filter according to Comparative Example 2 greatly exceed the upper limits shown in Tables 1 and 2.

For the optical filter according to Comparative Example 2, in both the near-infrared and ultraviolet regions, the boundary between a wavelength band of light expected to be transmitted and a wavelength band of light expected to be blocked is determined by light absorption. The light-reflecting layer exhibits its function of reflecting light by an interference effect attributed to its multilayer film. Thus, incidence of light at a large incident angle larger than a design value results not only in a shift of a wavelength band of reflected light to the short wavelength side but also in a ripple in a wavelength band of light which should be transmitted and severe distortion of the resultant spectral transmittance curve. For the optical filter according to Comparative Example 2, a narrow absorption band achieved by the light-absorbing layer in the near-infrared region results in failure to set the blocking band achieved by the light-reflecting layer on a sufficiently long wavelength side. Thus, the influence of the shift of the reflection band to the short wavelength side with increase in incident angle of light is inevitable for the optical filter according to Comparative Example 2. As a result, although the transmittance spectrum of light vertically incident on the optical filter according to Comparative Example 2 satisfies the desired requirements, the transmittance spectra of light incident thereon at larger incident angles cannot satisfy the desired requirements. When an imaging apparatus in which the optical filter according to Comparative Example 2 is incorporated is used to take an object at a wide angle of view, for example, for a wide-angle shot, it is difficult to reproduce an even color tone of the object in the image taken and there is also concern that the image obtained may be colored quite unevenly.

TABLE 3 (1) Spectral transmittance at wavelength of 380 nm 1.0% (2) Spectral transmittance at wavelength of 450 nm 81.4% (3) Average of spectral transmittance in wavelength 86.0% range of 500 nm to 600 nm (4) Spectral transmittance at wavelength of 700 nm 2.3% (5) Spectral transmittance at wavelength of 715 nm 0.8% (6) Average of spectral transmittance in wavelength 0.3% range of 700 nm to 800 nm (7) Maximum of spectral transmittance in wavelength <0.2% range of 750 nm to 1080 nm (8) Maximum of spectral transmittance in wavelength <0.2% range of 1000 nm to 1100 nm (9) Wavelength bandwidth in which spectral 177 nm transmittance is 75% or more between wavelengths of 400 nm and 700 nm

TABLE 4 ΔTs^(0/y)W-V y = 30° y = 35° y = 40° y = 45° y = 50° y = 55° y = 60° y = 65° W = 380 nm; V = 530 nm   0.8%   1.0% 1.2% 1.9% 2.0% 1.8% 2.8% 4.1% W = 450 nm; V = 650 nm   0.4%   0.6% 0.7% 1.1% 1.2% 1.3% 2.2% 2.7% W = 530 nm; V = 750 nm   0.6%   0.8% 1.1% 1.4% 1.5% 1.9% 2.6% 3.2% W = 650 nm; V = 1200 nm <0.2% <0.2% 0.2% 0.3% 0.3% 0.3% 0.4% 0.5% W = 380 nm; V = 1200 nm   0.3%   0.4% 0.5% 0.7% 0.8% 0.8% 1.2% 1.6%

TABLE 5 ΔTs^(30/y)W-V y = 35° y = 40° y = 45° y = 50° y = 55° y = 60° y = 65° W = 380 nm; V = 530 nm   0.2%   0.5%   1.1%   1.2% 1.3% 2.2% 3.3% W = 450 nm; V = 650 nm <0.2%   0.3%   0.6%   0.7% 1.0% 1.9% 2.3% W = 530 nm; V = 750 nm   0.2%   0.5%   0.7%   0.9% 1.3% 1.9% 2.6% W = 650 nm; V = 1200 nm <0.2% <0.2% <0.2% <0.2% 0.2% 0.3% 0.4% W = 380 nm; V = 1200 nm <0.2%   0.2%   0.4%   0.5% 0.6% 0.9% 1.3%

TABLE 6 (1) Spectral transmittance at wavelength of 380 nm 17.3% (2) Spectral transmittance at wavelength of 450 nm 83.6% (3) Average of spectral transmittance in wavelength 85.6% range of 500 nm to 600 nm (4) Spectral transmittance at wavelength of 700 nm 2.2% (5) Spectral transmittance at wavelength of 715 nm 0.8% (6) Average of spectral transmittance in wavelength 0.4% range of 700 nm to 800 nm (7) Maximum of spectral transmittance in wavelength 1.0% range of 750 nm to 1080 nm (8) Maximum of spectral transmittance in wavelength 1.6% range of 1000 nm to 1100 nm (9) Wavelength bandwidth in which spectral 192 nm transmittance is 75% or more between wavelengths of 400 nm and 700 nm

TABLE 7 ΔTs^(0/y)W-V y = 30° y = 35° y = 40° y = 45° y = 50° y = 55° y = 60° y = 65° W = 380 nm; V = 530 nm   0.4% 0.5% 0.6% 0.6% 1.0% 2.0% 3.6% 4.5% W = 450 nm; V = 650 nm   0.5% 0.5% 0.7% 0.9% 1.1% 1.3% 1.8% 2.2% W = 530 nm; V = 750 nm   0.6% 0.7% 1.0% 1.3% 1.5% 1.7% 1.8% 1.9% W = 650 nm; V = 1200 nm <0.2% 0.3% 0.3% 0.4% 0.5% 0.5% 0.6% 0.6% W = 380 nm; V = 1200 nm   0.3% 0.4% 0.5% 0.6% 0.7% 1.0% 1.3% 1.5%

TABLE 8 ΔTs^(30/y)W-V y = 35° y = 40° y = 45° y = 50° y = 55° y = 60° y = 65° W = 380 nm; V = 530 nm <0.2%   0.3% 0.4% 0.7% 1.6% 3.2% 4.0% W = 450 nm; V = 650 nm <0.2%   0.3% 0.5% 0.7% 0.9% 1.3% 1.7% W = 530 nm; V = 750 nm <0.2%   0.4% 0.7% 1.0% 1.2% 1.3% 1.4% W = 650 nm; V = 1200 nm <0.2% <0.2% 0.2% 0.3% 0.4% 0.4% 0.4% W = 380 nm; V = 1200 nm <0.2%   0.2% 0.3% 0.5% 0.7% 1.0% 1.2%

TABLE 9 (1) Spectral transmittance at wavelength of 380 nm 1.5% (2) Spectral transmittance at wavelength of 450 nm 78.5% (3) Average of spectral transmittance in wavelength 85.0% range of 500 nm to 600 nm (4) Spectral transmittance at wavelength of 700 nm 4.8% (5) Spectral transmittance at wavelength of 715 nm 2.2% (6) Average of spectral transmittance in wavelength 0.9% range of 700 nm to 800 nm (7) Maximum of spectral transmittance in wavelength 0.4% range of 750 nm to 1080 nm (8) Maximum of spectral transmittance in wavelength 0.7% range of 1000 nm to 1100 nm (9) Wavelength bandwidth in which spectral 173 nm transmittance is 75% or more between wavelengths of 400 nm and 700 nm

TABLE 10 ΔTs^(0/y)W-V y = 30° y = 35° y = 40° y = 45° y = 50° y = 55° y = 60° y = 65° W = 380 nm; V = 530 nm 0.8% 0.9% 1.1% 1.5% 1.9% 2.2% 2.5% 2.9% W = 450 nm; V = 650 nm 0.3% 0.5% 0.6% 0.7% 0.9% 1.0% 1.1% 1.2% W = 530 nm; V = 750 nm 0.6% 0.8% 1.0% 1.2% 1.4% 1.6% 1.7% 1.8% W = 650 nm; V = 1200 nm 0.2% 0.3% 0.3% 0.4% 0.4% 0.5% 0.5% 0.5% W = 380 nm; V = 1200 nm 0.3% 0.4% 0.5% 0.7% 0.8% 0.9% 1.0% 1.0%

TABLE 11 ΔTs^(30/y)W-V y = 35° y = 40° y = 45° y = 50° y = 55° y = 60° y = 65° W = 380 nm; V = 530 nm <0.2%   0.4%   0.7% 1.1% 1.4% 1.7% 2.1% W = 450 nm; V = 650 nm <0.2%   0.3%   0.4% 0.6% 0.7% 0.7% 0.9% W = 530 nm; V = 750 nm   0.2%   0.5%   0.7% 0.9% 1.0% 1.1% 1.2% W = 650 nm; V = 1200 nm <0.2% <0.2% <0.2% 0.2% 0.3% 0.3% 0.3% W = 380 nm; V = 1200 nm <0.2%   0.2%   0.3% 0.5% 0.6% 0.7% 0.7%

TABLE 12 (1) Spectral transmittance at wavelength of 380 nm <0.2% (2) Spectral transmittance at wavelength of 450 nm 82.5% (3) Average of spectral transmittance in wavelength 89.5% range of 500 nm to 600 nm (4) Spectral transmittance at wavelength of 700 nm 1.9% (5) Spectral transmittance at wavelength of 715 nm 0.7% (6) Average of spectral transmittance in wavelength 0.3% range of 700 nm to 800 nm (7) Maximum of spectral transmittance in wavelength 0.6% range of 750 nm to 1080 nm (8) Maximum of spectral transmittance in wavelength 0.9% range of 1000 nm to 1100 nm (9) Wavelength bandwidth in which spectral 183 nm transmittance is 75% or more between wavelengths of 400 nm and 700 nm

TABLE 13 ΔTs^(0/y)W-V y = 30° y = 35° y = 40° y = 45° y = 50° y = 55° y = 60° y = 65° W = 380 nm; V = 530 nm 0.8% 1.1% 1.3% 1.5% 1.6% 1.6% 1.6% 1.9% W = 450 nm; V = 650 nm 0.8% 1.1% 1.4% 1.7% 2.0% 2.2% 2.4% 2.7% W = 530 nm; V = 750 nm 0.9% 1.2% 1.6% 2.0% 2.5% 2.9% 3.2% 3.4% W = 650 nm; V = 1200 nm 0.3% 0.4% 0.5% 0.6% 0.7% 0.8% 0.9% 0.9% W = 380 nm; V = 1200 nm 0.5% 0.6% 0.8% 1.0% 1.2% 1.3% 1.4% 1.6%

TABLE 14 ΔTs^(30/y)W-V y = 35° y = 40° y = 45° y = 50° y = 55° y = 60° y = 65° W = 380 nm; V = 530 nm   0.3%   0.6% 0.8% 1.1% 1.2% 1.2% 1.3% W = 450 nm; V = 650 nm   0.3%   0.7% 1.1% 1.4% 1.7% 1.9% 2.1% W = 530 nm; V = 750 nm   0.3%   0.7% 1.2% 1.6% 2.0% 2.3% 2.6% W = 650 nm; V = 1200 nm <0.2% <0.2% 0.3% 0.4% 0.5% 0.6% 0.6% W = 380 nm; V = 1200 nm <0.2%   0.4% 0.6% 0.7% 0.9% 1.0% 1.1%

TABLE 15 (1) Spectral transmittance at wavelength of 380 nm <0.2% (2) Spectral transmittance at wavelength of 450 nm 86.2% (3) Average of spectral transmittance in wavelength 90.2% range of 500 nm to 600 nm (4) Spectral transmittance at wavelength of 700 nm 1.4% (5) Spectral transmittance at wavelength of 715 nm 0.3% (6) Average of spectral transmittance in wavelength 0.3% range of 700 nm to 800 nm (7) Maximum of spectral transmittance in wavelength 0.7% range of 750 nm to 1080 nm (8) Maximum of spectral transmittance in wavelength 0.5% range of 1000 nm to 1100 nm (9) Wavelength bandwidth in which spectral 196 nm transmittance is 75% or more between wavelengths of 400 nm and 700 nm

TABLE 16 ΔTs^(0/y)W-V y = 30° y = 35° y = 40° y = 45° y = 50° y = 55° y = 60° y = 65° W = 380 nm; V = 530 nm 6.9% 10.2% 12.7% 15.3% 17.6% 19.0% 20.4% 22.5% W = 450 nm; V = 650 nm 1.7%  2.6%  4.0%  7.2% 11.7% 16.3% 21.0% 25.1% W = 530 nm; V = 750 nm 2.3%  3.3%  4.8%  7.0%  9.7% 12.5% 15.6% 18.3% W = 650 nm; V = 1200 nm 1.2%  2.0%  3.0%  4.1%  5.6%  6.9%  8.5% 11.0% W = 380 nm; V = 1200 nm 2.3%  3.5%  4.7%  6.3%  8.4% 10.2% 12.3% 15.2%

TABLE 17 ΔTs^(30/y)W-V y = 35° y = 40° y = 45° y = 50° y = 55° y = 60° y = 65° W = 380 nm; V = 530 nm 4.1% 8.1% 12.4% 16.3% 18.4% 19.6% 20.0% W = 450 nm; V = 650 nm 1.9% 3.5%  6.3% 11.2% 15.6% 20.0% 24.2% W = 530 nm; V = 750 nm 1.6% 3.2%  5.1%  7.9% 10.7% 13.5% 16.4% W = 650 nm; V = 1200 nm 0.9% 1.9%  3.0%  4.6%  5.9%  7.4% 10.0% W = 380 nm; V = 1200 nm 1.5% 3.1%  4.9%  7.3%  9.3% 11.3% 13.9%

TABLE 18 (1) Spectral transmittance at wavelength of 380 nm <0.2% (2) Spectral transmittance at wavelength of 450 nm 84.6% (3) Average of spectral transmittance in wavelength 87.1% range of 500 nm to 600 nm (4) Spectral transmittance at wavelength of 700 nm 1.3% (5) Spectral transmittance at wavelength of 715 nm 0.3% (6) Average of spectral transmittance in wavelength 0.2% range of 700 nm to 800 nm (7) Maximum of spectral transmittance in wavelength <0.2% range of 750 nm to 1080 nm (8) Maximum of spectral transmittance in wavelength <0.2% range of 1000 nm to 1100 nm (9) Wavelength bandwidth in which spectral 172 nm transmittance is 75% or more between wavelengths of 400 nm and 700 nm

TABLE 19 ΔTs^(0/y)W-V y = 30° y = 35° y = 40° y = 45° y = 50° y = 55° y = 60° y = 65° W = 380 nm; V = 530 nm 1.9% 3.2% 5.4% 8.1% 10.8% 13.9% 16.7% 17.7% W = 450 nm; V = 650 nm 1.7% 2.4% 4.2% 7.5% 11.0% 15.3% 19.9% 22.2% W = 530 nm; V = 750 nm 1.9% 2.8% 4.3% 6.5%  8.6% 11.2% 14.2% 16.4% W = 650 nm; V = 1200 nm 0.7% 1.2% 1.8% 2.2%  2.7%  3.1%  3.3%  3.9% W = 380 nm; V = 1200 nm 1.0% 1.6% 2.5% 3.7%  5.0%  6.5%  8.0%  9.1%

TABLE 20 ΔTs^(30/y)W-V y = 35° y = 40° y = 45° y = 50° y = 55° y = 60° y = 65° W = 380 nm; V = 530 nm 2.2% 4.3% 6.8%  9.8% 13.0% 15.6% 17.0% W = 450 nm; V = 650 nm 1.7% 3.4% 6.2% 10.1% 14.5% 18.8% 21.4% W = 530 nm; V = 750 nm 1.3% 2.8% 4.6%  6.8%  9.5% 12.4% 14.6% W = 650 nm; V = 1200 nm 0.5% 1.1% 1.5%  2.1%  2.4%  2.7%  3.2% W = 380 nm; V = 1200 nm 0.9% 1.8% 2.9%  4.2%  5.7%  7.2%  8.3% 

The invention claimed is:
 1. An optical filter comprising: a light-absorbing layer that includes a light absorber for absorbing light in at least a portion of the near-infrared region, wherein when light with a wavelength of 300 to 1200 nm is incident on the optical filter at an incident angle of 0°, the optical filter satisfies the following requirements (1) to (9): (1) a spectral transmittance at a wavelength of 380 nm is 20% or less; (2) the spectral transmittance at a wavelength of 450 nm is 75% or more; (3) an average of the spectral transmittance in the wavelength range of 500 to 600 nm is 80% or more; (4) the spectral transmittance at a wavelength of 700 nm is 5% or less; (5) the spectral transmittance at a wavelength of 715 nm is 3% or less; (6) an average of the spectral transmittance in the wavelength range of 700 to 800 nm is 1% or less; (7) the maximum of the spectral transmittance in the wavelength range of 750 to 1080 nm is 1% or less; (8) the maximum of the spectral transmittance in the wavelength range of 1000 to 1100 nm is 2% or less; and (9) a wavelength bandwidth of a wavelength band in which the spectral transmittance in the wavelength range of 400 to 700 nm is 75% or more is 170 nm or more, when light with a wavelength of 300 to 1200 nm is incident on the optical filter at incident angles of x° and y° (0≤x≤30, 30≤y≤65, and x<y) and an average of absolute values of differences each between a value of a normalized spectral transmittance for the incident angle x° and a value of a normalized spectral transmittance for the incident angle y° at the same wavelength in the wavelength range of W nm to V nm (W<V) is expressed as ΔT_(S) ^(x/y) _(W-V), the optical filter satisfies requirements ΔT_(S) ^(0/40) ₃₈₀₋₅₃₀≤3%, ΔT_(S) ^(0/40) ₄₅₀₋₆₅₀≤3%, and ΔT_(S) ^(0/40) ₅₃₀₋₇₅₀≤3%, the normalized spectral transmittance being determined by normalization of a spectral transmittance for each of the incident angles so that the maximum of the spectral transmittance for each of the incident angles in the wavelength range of 400 to 650 nm is 100% and ΔT_(S) ^(0/v) ₃₈₀₋₅₃₀ is 1.9% or less when y is in the range of 35 to
 65. 2. The optical filter according to claim 1, wherein the optical filter further satisfies a requirement ΔT_(S) ^(0/40) ₆₅₀₋₁₂₀₀≤1%.
 3. The optical filter according to claim 1, wherein the optical filter further satisfies a requirement ΔT_(S) ^(0/40) ₃₈₀₋₁₂₀₀≤1.5%.
 4. The optical filter according to claim 1, wherein the optical filter further satisfies requirements ΔT_(S) ^(0/50) ₃₈₀₋₅₃₀≤4%, ΔT_(S) ^(0/50) ₄₅₀₋₆₅₀≤4%, ΔT_(S) ^(0/50) ₅₃₀₋₇₅₀≤4%, ΔT_(S) ^(0/50) ₆₅₀₋₁₂₀₀≤1.5%, and ΔT_(S) ^(0/50) ₃₈₀₋₁₂₀₀≤2%.
 5. The optical filter according to claim 1, wherein the optical filter further satisfies requirements ΔT_(S) ^(0/60) ₃₈₀₋₅₃₀≤4.5%, ΔT_(S) ^(0/60) ₄₅₀₋₆₅₀≤4.5%, ΔT_(S) ^(0/60) ₅₃₀₋₇₅₀≤4.5%, ΔT_(S) ^(0/60) ₆₅₀₋₁₂₀₀≤1.5%, and ΔT_(S) ^(0/60) ₃₈₀₋₁₂₀₀≤2.5%.
 6. The optical filter according to claim 1, wherein the optical filter further satisfies requirements ΔT_(S) ^(0/65) ₃₈₀₋₅₃₀≤5%, ΔT_(S) ^(0/65) ₄₅₀₋₆₅₀≤5%, ΔT_(S) ^(0/65) ₅₃₀₋₇₅₀≤5%, ΔT_(S) ^(0/65) ₆₅₀₋₁₂₀₀≤1.5%, and ΔT_(S) ^(0/65) ₃₈₀₋₁₂₀₀≤3%.
 7. The optical filter according to claim 1, wherein the optical filter further satisfies requirements ΔT_(S) ^(30/40) ₃₈₀₋₅₃₀≤3%, ΔT_(S) ^(30/40) ₄₅₀₋₆₅₀≤3%, ΔT_(S) ^(30/40) ₅₃₀₋₇₅₀≤3%, ΔT_(S) ^(30/40) ₆₅₀₋₁₂₀₀≤1%, and ΔT_(S) ^(30/40) ₃₈₀₋₁₂₀₀≤1.5%.
 8. The optical filter according to claim 1, wherein the optical filter further satisfies requirements ΔT_(S) ^(30/50) ₃₈₀₋₅₃₀≤3%, ΔT_(S) ^(30/50) ₄₅₀₋₆₅₀≤3%, ΔT_(S) ^(30/50) ₅₃₀₋₇₅₀≤3%, ΔT_(S) ^(30/50) ₆₅₀₋₁₂₀₀≤1%, and ΔT_(S) ^(30/50) ₃₈₀₋₁₂₀₀≤1.5%.
 9. The optical filter according to claim 1, wherein the optical filter further satisfies requirements ΔT_(S) ^(30/60) ₃₈₀₋₅₃₀≤4%, ΔT_(S) ^(30/60) ₄₅₀₋₆₅₀≤4%, ΔT_(S) ^(30/60) ₅₃₀₋₇₅₀≤4%, ΔT_(S) ^(30/60) ₆₅₀₋₁₂₀₀≤1.5%, and ΔT_(S) ^(30/60) ₃₈₀₋₁₂₀₀≤2%.
 10. The optical filter according to claim 1, wherein the optical filter further satisfies requirements ΔT_(S) ^(30/65) ₃₈₀₋₅₃₀≤4.5%, ΔT_(S) ^(30/65) ₄₅₀₋₆₅₀≤4.5%, ΔT_(S) ^(30/65) ₅₃₀₋₇₅₀≤4.5%, ΔT_(S) ^(30/65) ₆₅₀₋₁₂₀₀≤1.5%, and ΔT_(S) ^(30/65) ₃₈₀₋₁₂₀₀≤2.5%.
 11. The optical filter according to claim 1, wherein the light absorber is formed by a phosphonic acid and copper ion.
 12. The optical filter according to claim 11, wherein the phosphonic acid comprises a first phosphonic acid having an aryl group.
 13. The optical filter according to claim 12, wherein the phosphonic acid further comprises a second phosphonic acid having an alkyl group.
 14. An imaging apparatus comprising: a lens system; an imaging device that receives light having been transmitted through the lens system; and the optical filter according to claim 1 that is disposed ahead of the imaging device.
 15. The imaging apparatus according to claim 14 further comprising a color filter that is disposed ahead of the imaging device and is a filter of three colors, R (red), G (green), and B (blue), wherein the optical filter is disposed ahead of the color filter.
 16. The optical filter according to claim 1, further comprising: a first light-absorbing layer that includes a first light absorber comprising a copper ion and a first phosphonic acid with an aryl group, a second light-absorbing layer that includes a second light absorber comprising a copper ion and a second phosphonic acid with an alkyl group, and an ultraviolet-absorbing layer being capable of absorbing light in at least a portion of the ultraviolet region.
 17. The optical filter according to claim 16 further comprising: a SiO₂-containing layer that is disposed between the first light-absorbing layer and the second light-absorbing layer. 